cr> oa ID 3 < O' ax Q US > GJ a UJ 0$ CRNL-TM- 3793 MASTER JOB STREAM OF CASES FOR THE COMPUTER CODE CITATION D. R. Vondy and T. B. Fowler 7\- +» , T V ■ !i * *• "**■ ' I OAK RIDGE NATIONAL LABORATORY OPERATEO BY , UNION. CARBIDE GOS^ORAtlOjj • FOR ’ .HE U.S. ATOMIC ENERGY COMMISSION I ’ v •v \ - i . > \* ■
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C R N L-T M - 3793
MASTERJOB STREAM OF CASES FOR THE
COMPUTER CODE CITATION
D. R. V o n d y a n d T. B. Fowler
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OAK RIDGE NATIONAL LABORATORYOPERATEO BY, UNION . CARBIDE GOS ORAtlOjj • FOR ’ .HE U.S. ATOMIC ENERGY COMMISSION
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ORNL-TM-3793
Contract No. W-7405--eng-26
REACTOR DIVISION
JOB STREAM OF CASES FOR THE COMPUTER CODE CITATION
D. R. Vondy and T. B. Fowler
----------------------------------------N O T I C E ----------------------------------------This report was prepared as an account o f work sponsored by the United States Government. Neither the United States nor the United States Atom ic Energy Commission, nor any o f their employees, nor any of their contractors, subcontractors, or their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, com pleteness or usefulness o f any information, apparatus, product or process disclosed, or represents that its use w ould not infringe privately owned rights.
JULY 1972
NOTICE This document contains information of a preliminary nature and was prepared primarily for internol use at the Oak Ridge National Laboratory. It is subject to revision or correction and therefore does not represent a final report.
OAK RIDGE NATIONAL LABORATORY Oak Ridge, Tennessee 37830
operated by UNION CARBIDE CORPORATION
for theU.S. ATOMIC ENERGY COMMISSION
WSTRWUTON Of THIS &©CDME!|T IS IML
3
CONTENTS
Page
Abstract .............................................................. 1
Introduction .......................................................... 5
1. Three Cases: One Dimensional Slab, Cylinder and Sphere . , . 6
2. Three Cases: A Two-Dimensional Perturbation Calculationwith Results of Perturbed Cases for Comparison ............. 8
3. Two-Dimensional Fixed Source Without Fission Source ......... 9
Two-Dimensional Fixed Source Problem ■with Fission Source . . 9
5. Two-Dimensional Search on Absorber .......................... 9
6. Two-Dimensional Fast Reactor Dimension Search . . . . . . . . 1 0
7. Three Cases: A Reference Case with Reflected Boundaries andThen Two Cases with the Periodic Boundary Condition ........ 10
8. Two Cases: R-Z Geometry Followed by a Theta-R-Z Case . . . . 11
9. Two Cases: Triagonal Three-Dimensional Case Followed by aSimilar Theta-R-Z C a s e ..................................... 11
10. Hexagonal Three-Dimensional C a s e ........................... 12
11. Three-Dimensional FFTF Case in Reduced F o r m ................ 12
12. Three-Dimensional Case Called C l a g ..................... .. . 12
13* Three-Dimensional Buckling Search........................... 13
1^. Two Cases: Treatment of 90 Degree Rotational Symmetry Followedby the Same Problem Run with 180 Degree Rotational Symmetry . 13
15. Ficticious Plutonium Exposure Given a Fixed Source ......... 1^
16. Multi-Cycle Breeder Fuel Management C a s e ............... . . 1^
References ........... ............................................. 297
BLANK
ABSTRACT
A series of cases is described, input data requirements given and results reported, for the CITATION computer code which applies finite-difference diffusion theory in up to three space dimensions.
These are reference problems which collectively exercise many different options programmed in this code, and therefore serve to verify proper implementation of it. Included are non-dimensional, one-, two-, and three-dimensional eigenvalue problems of various kinds, fixed source problems, and sophisticated fuel management problems carried through several fuelings. Not only is the capability for criticality search exploited, but for several cases the adjoint eigenvalue problem is also solved and first-order perturbation results obtained and reported.
Key Words: mathematics, computer code, reactor calculations, ones
5
JOB STREAM OF CASES FOR THE COMPUTER CODE CITATION
D. R. Vondy and T. B. Fowler
INTRODUCTION
Contacts with individuals implementing the CITATION code on a variety
of computers have shown us the critical need for a set of reference prob
lems. Only by running a series of problems of great variety, exercising
various options, can the integrity of a complicated computer code be
established. After major c o d e changes we have run such a job stream of
cases, (indeed the set of cases included would have proven superior for
testing to the set which we have used in the past). '
Of critical importance is checking integrity when there are differences
from the normal operation employed by the originators. Errors in each com
piler have to be programmed around, for example. Certain changes in the
source language are necessary in converting to operation on a different
type of computer. Operating systems behave differently. Taking these
factors together, the implementor of a code in an environment foreign to
that of the originators is faced with some of the same problems as the
originators: obtaining correct results in spite of the facility, and
tailoring the program to his environment. For any code transmitted, a
sample problem is of course essential. A variety of problems with reliable
solutions is also deemed essential when they exercise various combinations
of the major programmed options in such a way as to provide a reasonable
test of the integrity of an implementation. r
. These cases were set up to serve a specific function. They do indeed
indicate capability of the CITATION code. They are designed to test the
code and may not represent realistic analysis of specific nuclear reactors.
They do not replace the sample problem reported, but extend it.
The input data and results reported are compatible with the most recent
release of the CITATION code and its reference document, ORNL-TM-2U96 dated
(as revised) March 1972.
In this report, each individual case, or series of related cases, is
discussed. The problem description is brief and refers both to the input
6
data presented in Table 1 and the edit associated with the input data in
Table 2. Special features of the individual cases are given attention.
Then the results are discussed as appropriate. This stream of cases
required 10 minutes CPU time on the IBM 360/91 computer.
Given below is a list of the cases, often sets of cases, covered by
memorandum.
1. Three cases: one-dimensional slab, cylinder and sphere.
2. Three cases: a two-dimensional perturbation calculation with
results of perturbed cases for comparison.
3. Two-dimensional fixed source without fission source.
k. Two-dimensional fixed source problem with fission source.
5. Two-dimensional search on absorber.
6. Two-dimensional fast reactor dimension search.
7* Three cases: a reference case with reflected boundaries and
then two cases with the periodic boundary condition.
8. Two cases: R-Z geometry followed by a Theta-R-Z case.
9. Two cases: triagonal three-dimensional case followed by a
similar Theta-R-Z case.
10. Hexagonal three-dimensional case.
11. Three-dimensional FFTF case in reduced form.
12. Three-dimensional case called CLAG.
13. Three-dimensional buckling search.
1^. Two cases: treatment of 90 degree rotational symmetry followed
by the same problem run with 180 degree rotational symmetry.
15. Fictitious plutonium exposure given a fixed source.
16. Multi-cycle breeder fuel management case.
1. THREE CASES: 01® DIMENSIONAL SLAB, CYLINDER AND SPHERE
These one-dimensional traverses are for systems which are similar in
a nuclear sense. The same seven group cross sections are used for the
cases and each has 2b mesh points in ’Jhe core and 10 mesh points in the
inactive blanket. In each case both the forward and adjoint neutron flux
problems are solved and results of the usual forward-adjoint intergrals
for a first-order perturbation theory analysis are reported.
7
Regarding the input data, the first case has a full set of data,'
the title cards followed by the sections in order 001, 003, 00 , 005,
008 giving macroscopic data, 012 identifying zones, 02*+ buckling, and
0^0 perturbation data, with a 999 card closure. The second case has only
sections 001 changing the edit options, 003 changing the geometry, and
00^ changing the mesh spacing. The third case replaces only the data in
sections 003 and OOH.
Note that the macroscopic data supplied in section 008 is edited for
the first case. The data actually used for the calculation is slightly
different. Total loss cross sections are calculated (sum of the outscat-
tering, absorption and buckling loss) for each zone. From this is subtracted
the sum of everything except absorption; this leaves an effective absorption
cross section consistent with short word precision use of the data, a little
"hanky panky" usually having no significant effect on the data used.
Examination of the interative process in resolution of the neutron
flux eigenvalue problems shows that overrelaxation is not done for one
dimensional problems (the overrelaxation coefficient BETA is unity) since
at each energy each successive estimate of the fluxes is a simultaneous
solution alonn, the line. The extrapolation procedure is seen to be ef
fective. Note the vast improvement in the estimate of the multiplication
factor, K after extrapolation in each case and the decrease in the error
bounding maximum relative FLUX CHANGE between iterations. Estimates of
the eigenvalue of the predominating error mode from point flux value
changes are MU-1 and MU-2, while MU-3 is an independent value from an .
integral quantity which has not proven useful. The estimate of K from
the forward problem is used for the adjoint problem and not reevaluated.
Upon termination of the iterative process when convergence criteria have
been satisfied, an independent estimate of K and also the value of a
multiplier on all absorption cross sections are determined, values which
each would minimize the sum of the squares of the residues of the point
neutron balance equations. Thus three estimates of K are available here:
Method Slab Cylinder Sphere
Neutron Balance ResiduesAdjoint Residues
0.8939080.8939350.8939*11
O.87OI680.8701790.870213
0.8595770.8595850.859615
Averages 0.893928 O.87OI87 0.859592
8
The values are seen to be in agreement in each case to less than the
specified maximum relative point flux change (CITATION code default value)
of 0.0001.
The GROSS NEUTRON BALANCE obtained by input option for each case is
for the forward problem. Individual contributions to an overall neutron
balance are shown by energy group in a general table which is arranged for
up to three space dimensions. There is no buckling nor l/v loss, and we
have not advanced to the stage of obtaining a XENON LOSS. OUT-SCATTER is
from that group to all others, IN-SCATTER is from all other groups to that
one (no in-group scatter considered), the SOURCE values are the TOTAL
PRODUCTIONS divided by K distributed by CHI. If fully converged, TOTAL
LOSSES would equal TOTAL GAINS by energy group. The PROD/ABSORP is a
’'macroscopic average eta" indicating the ratio of neutrons produced to
neutrons absorbed.
The reader may also note that at the start of the edited results, the
version of the CITATION program in use is identified, the date is given
and the computer model is shown. Following the information about the
iterative process for each eigenvalue problem, the computer central proces
sor unit (CPU) time required for solving the problem (not including proces
sing input data nor setting up the problem) is given. At the end of each
case a normal termination is indicated along with both the CPU time and
total clock (real) time. This computer run used only a small amount of the
fast memory of the computer, 100,000 short words of the available 393^216.
Under multi-tasking, other jobs were also being processed, so the CPU time
is naturally much less than the total time and the CPU efficiency can not
be determined from the available information.
2. THREE CASES: A TWO-DIMENSIONAL PERTURBATION CALCULATION WITH RESULTS OF PERTURBED CASES FOR COMPARISON
This small problem is one we have used for years to check out pertur
bation calculations. The two-dimensional problem is first solved, then the
adjoint problem is solved, and first-order perturbation results obtained
as requested. Note that a neutron balance by energy group is also reported
for each of the three zones along with average neutron flux values and
volumes, and the power density map is edited. For the next case the
9
diffusion constant for the first group and first zone is changed from
0.500028 to 0.1+50028, and in the last case it is specified as 0.25G0lk. A comparison of the results follows.
As the perturbation is increased, the change in the multiplication
factor deviates more from the first-order perturbation result which is
precise only in the limit of no change.
3. TWO-DIMENSIONAL FIXED SOURCE WITHOUT FISSION SOURCE
This little one-group fixed source problem was extracted from one
presented in the literature.1 Luring the iterative process the level of
the fixed source is adjusted at each iteration to satisfy an overall
neutron balance, and on termination the neutron flux values ere renormalized
to the original source strength. Contained with the iterati- 5 information
is an overall neutron balance which shows how the imb^ ancr is reduced. One
of the few edits of point neutron flux values was obtained for this problem.
b. TWO-DIMENSIONAL FIXED SOURCE PROBLEM WITH FISSION SOURCE
This is another one-group fixed source problem, but hezc there is a
value for providing a flux-dependent fission source. The flux edit
indicates that the diagonal symmetry presented no difficulty; only slight
disagreement is found in the fourth digit of the flux values at points of
symmetry.
This problem treats seven groups with upscatterjng, a two-dimensional
bare slab. The calculation is a direct oriticality search, iteration
toward a desired multiplication factor by adjusting the absorption cross
sections. The search factor obtained must be subtracted from unity to
give the value of relative absorption cross section because of the way
the actual cross sections were used as l/v data: 1 .0 — 0.256956 ~ 0.7^30^ .
This result compares with a precise value of 0.7376078371 for a continum.2
Case keff
0.185920.186830.19111
dk/kdD
Reference, Perturbation D (1, 1) Changed -0.05 D (l, l) Changed —0.25001^
~0.08J-'99-0.098-0.110
5. TWO-DIMENSIONAL SEARCH ON ABSORBER
10
An interesting aspect is how well, this problem is accelerated by extrap
olation; significant reduction from the error mode predominating asymp
totically is achieved by extrapolation.
6. TWO-DIMENSIONAL. FAST REACTOR DIMENSION SEARCH
This case is the first to use microscopic cross sections; they are
supplied in input section 000, an 012 section is necessary for assignments
(and applies names to sets of zones), and nuclide concentrations (DENSITIES)
must be provided by zone (or series of zones) in an 020 section. A section
028 of input data is also included to direct the search on dimensions.
In the edit is information about the generation of a cross section
library. Following the DESCRIPTION OF REACTOR ZONES is a DESCRIPTION OF
MICROSCOPIC CROSS SECTIONS which presents such reference information as
needed to document the data (15 nuclides, 5 energy groups, group energies,
l/v data and the source distribution function).
According to the input data specifications, the spacings associated
with the first 19 mesh points along the X coordinate are to have unit
changes while those of the last 9 mesh points along the Y coordinate are
to be changed half as much in satisfying a desired multiplication factor
of 0.95* The solution of the initial eigenvalue problem gave a
kgff = 1.01137* Then a change was made in the mesh, a decrease to reduce
keff, and the result obtained after a single iteration of the problem was
used to adjust the first change, to effect a reasonable step out in the
space dimension variable. Then the outer-iteration procedure was applied
to bring the problem to an acceptable solution. An edit of the final
spacial mesh is presented, and also certain damage rate data, a summary
of neutron losses, and fissile conversion and power and fissile loading
distributions.
7- THREE CASES: A REFERENCE CASE WITH REFLECTED BOUNDARIES AND THEN TWO CASES WITH THE PERIODIC BOUNDARY CONDITION
These cases provide a check of the treatment of the periodic boundary
condition applied to zones of black absorption. We have heard of some dif
ficulty in understanding the layout of Theta-R geometry. The center of
the circle goes to the top. The left boundary is along a radius, there
is a false (nonexisting) boundary at the top (must be reflecting), the
11
right boundary is along another radius, and closure is along the bottom
boundary. Ficticious regions or points required by several older codes
have been entirely eliminated in CITATION so that only real boundaries
need be considered.
Comparison of the results of the perturbation calculations for the
first and third problems in this set shows three digit agreement.
8. TWO CASES: R-Z GEOMETRY FOLLOWED BY A THETA-R-Z CASE
These cases provide a direct, coarse check of the treatment of three
dimensional geometry involving the Theta dimension with the periodic
boundary condition. The third dimension (Theta) is simply added so that
a flat flux along it results. A comparison of the cases may be informative
about mocking up problems involving the Theta dimension. Most of the first
order perturbation results '(integrals) show three digit significance, but
two significant figures are not guaranteed by the level of convergence
specified.
9. TWO CASES: TRIAGONAL THREE-DIMENSIONAL CASE FOLLOWED BY ASIMILAR THETA-R-Z CASE
Triagonal geometry is of special interest for treating hexagonal as
semblies of fuel pins. This case also demonstrates a usefulness of the
black absorber approximation: a suitable boundary condition may be placed
inside a geometric mesh by defining a zone to be a black absorber which
has an extrapolated flux boundary condition extending into the absorber.
This use of the black absorber condition in all energy groups has appli
cation even in fast reactor analysis.
When the black absorber condition is applied in all groups in a zone,.
all cross sections for this zone are set to zero, and at all points internal
to this zone the neutron flux values are set to zero. Absorption within
the black absorber region is determined from interface leakage.
To provide some additional information, results from several cases
which have been run but are not included here are reported below.
12
Spacial Meshpoints
Triagonal Z Total Keff
32 • k 128 0.7273128 k 512 0.7209288 k 1152 0.7197128 12 1536 O .6766128 20 2560 0.6731288 20 5760 0.6720
Clearly it takes more than four points along one dimension for a
reliable representation of the neutron flux.
The second case of this set is a mock up of the problem in Theta-R-Z
geometry with 128 points on a plane. However, these points are used to
represent only one-twelfth of the system compared with one-sixth treated
by the triagonal representation. Thus the result of keff = 0.7218 for
four points along Z is considered to be in reasonable agreement with the
results shown above. The perturbation results are not much different for
the two cases in spite of the different representations.
10. HEXAGONAL THREE-DIMENSIONAL CASE
This little case is included as a reference calculation in hexagonal
geometry. It should be noted that a single mesh point is located at the
center of each hexagon. Generally a finer mesh can not be used, and there
are serious constraints on application of this geometry because of the way
points are located off boundaries. Refer to the drawing in the code report
for a visual display of points and boundaries.
There are, however, special applications where this geometry is useful.
A coarse mock up of hexagonal assemblies is possible (one point per hexagon
compared with a minimum of six with triagonal geometry). It has also been
used for representing mixed systems, as cylinders in slabs.
11. THREE-DIMENSIONAL FFTF CASE IN REDUCED FORM
This case is a coarse representation of a reactor core under design.
12. THREE-DIMENSIONAL CASE CALLED CLAG .
This three-dimensional case was adopted by us for test purposes from
a Knolls Atomic Power Laboratory Report.3 The case has diagonal symmetry,
13
unknown to the code. The degree of symmetry in the results is a measure
of convergence of the problem.
Of interest in this problem is the handling of the finite-difference
neutron balance equation constants. When feasible, these are all stored
in the fast memory. For the larger problems those constants representing
leakage coupling and total loss are input from disk by energy group during
the iterative process. For this case 38^60 words storage are required
with data input; without input the requirement for this four-energy group
problem is 6^070 words based on the edited information.
13. THREE-DIMENSIONAL BUCKLING SEARCH
The direct search procedure is used for this old WHIRLAWAY case to
satisfy a desired multiplication factor by adjusting the buckling. A
DB?£> loss is allowed in all geometries, even three-dimensional (such may
be useful for any problem, although occasionally a tenderfoot incorrectly
puts in the system buckling when the whole geometry is treated as a 1-D
sphere, 2-D cylinder or in 3-L).
To demonstrate user control, an overrelaxation factor is specified
for this case and the iterative process is done by the Direct Alternating-
Direct ion Line Overrelaxation (DALOR) sweeping along rows, then columns,
then fore and aft at each energy. Each point neutron flux value is deter
mined three times each outer iteration.
It is interesting to note that given a good flux shape, the! adjoint
problem quickly converges.
Ik. TWO CASES: TREATMENT OF 90 DEGREE ROTATIONAL SYMMETRY FOLLOWEDBY THE SAME PROBLEM RUN WITH 180 DEGREE ROTATIONAL SYMMETRY
These three-dimensional cases are used for a test of two special
boundary conditions. The 90 degree rotational symmetry condition involves
coupling the right column of points with the bottom row on each plane.
The 180 degree rotational symmetry case is twice as large and involves
coupling the right column of points with itself but inverted. These
special boundary conditions are useful for two situations:
(l) treating a core with a minimum number of points, especially
important when depletion is considered, and
lb
(2) the cell problem where explicit representation of a symmetry
condition causes much faster iteration and a significant
savings in computation time.
. The heat deposition in the coolant, per unit total cross rectional
area, is edited for the last case.
15. FICTITIOUS PLUTONIUM EXPOSURE GIVEN A FIXED SOURCE
This is a rather peculiar case. It is complicated because microscopic
cross sections for 240 Pu are correlated against concentration. It is
simple because the first "cycle" of exposure involves fixed source prob
lems (-with fission source). It demonstrates great flexibility because
a second "cycle" of exposure is done solving eigenvalue problems. We
include it here -without elaborate explanation as a test of several
features of the CITATION code.
This case does illustrate a recent addition to the code: the ability
to change microscopic cross section data during an exposure calculation.
As specified, an original set of data is replaced by another set, and
considerable flexibility during a cycle is allowed.
16. MULTI-CYCLE BREEDER FUEL MANAGEMENT CASE
Remarks
This case is a fairly involved treatment of a fast reactor breeder.
It is included here to supplement the sample problem distributed with
the CITATION code; the two cases are similar physically. The capability
demonstrated represents a significant investment in methods development.
Please note that the fuel management capability is available in all
geometries through three dimensions in the finite-difference representa
tion of diffusion theory.
Included below is a discussion about the fuel management treatment
and data requirements which follow this problem and supplement the
discussion in the code report.
15
General Description
This calculation simulates the operation of the reactor4 with re
fueling intervals of specified length. Initial parameters are adjusted
ai the beginning of each interval to achieve specified conditions during
the cycle. The parameter to be varied, in order to achieve the desired
condition of a minimum fractional loss to control poison, is the fraction
of fuel available for recycle which can actually be used each fueling,
the recycled fuel being distributed proportionately in each of the three
enrichment zones. After recycle, each fueling period (cycle) was recal
culated with adjustment of this "recycle fraction" until the specified
condition was met. The refueling interval was held fixed at 150 full-power
days. Information generated as the calculation proceeded, namely the
dependence of the fractional loss to control poison on the amount of fuel
recycled, permitted desired results to be achieved within a reasonable
amount of calculation time.
The neutronics problems considered three energy groups and 96 space
points, while there were two nondepleting and 20 depleting zones each
sub-divided into four subzones. Figure 1 shows the zone layout for this
problem. Exposure calculations were done for 80 fuel batches (loOO nuclide
concentrations). The exposure history between fuelings was done with
solution of three eigenvalue problems, i.e., at the start, mid-point, and
end of each refueling interval.
A criticality search was done on the smeared control poison, which
displaced sodium coolant, and the minimum fractional loss to this control
poison during each cycle was specified as 0.0025 - 0.000025.
Results of this calculation for 25 fuelings are shown in Table 1,
with the effectiveness of the programmed procedure demonstrated. The
code permits restart at any cycle of such cases provided the mesh, energy
groups, and zone description and are not changed. The input data for the
job stream case included carries this calculation through only 5 fuelings.
Detailed Description of Fuel Management and Input
A detailed description of the fuel management carried out by the
code is given here along with a description of the input data that
16
ORNL-DWG 72-5884
FOUR SUBZONES: FOUR SETS OF CONCENTRATIONS (SUB-ZONES) ARE
SPECIFIED FOR EACH ZONE 1 THROUGH 20
■INNER CORE
ZONE 1
- CLASS 1
ZONE 2
------AXIAL BLANKE"
ZONE 7
..... ....r 1 - CLASS 4
ZONE 8
REFLECTOR
- CLASS
10,
ZONE
22
MIDDLE COR
ZONE 3
• - CLASS 2
ZONE 4
AXIAL BLANKE'
ZONE 9
’ 2 - CLASS 5
ZONE 10
OUTER CORE
ZONE 5
- CLASS 3
ZONE 6
AXIAL BLANKE’
ZONE 11
r 3 - CLASS 6
ZONE 12
ZONE 13
INNER RADIAL BL
ZONE 14
ANKET - CLASS 7
ZONE 15 ZONE 16
ZONE 17
OUTER RADIAL BL
ZONE 18
W K E T - CLASS 8
ZONE 19 ZONE 20
REFLECTOR - CLASS 9, ZONE 21
Figure 1. Zone Layout for Fuel Management Problems.
17
Table 1. Results for 25 Fuelings
Fueling(Cycle)
Fraction of Available Plutonium Recycled
Minimum Fraction Absorption
in Control Poison
End of Exposure Fissile Loading (kg)
1 — — — 3322
2 - - ---- 3 ^ 3
3 1.0000 0.0221+8 3552
0.9000 0.00587 31+88
0.8797 0.00239 3V76
. 0.8803 0.00250 31*76
k 0.8803 -0.00538 35130.926k 0.00289 35^30.921+2 0.00251 35M
5 0.921+2 0.00761 360k
0.8958 0.0021+1+ 35850.8961 0.00250 3585
6 0.8961 0.00708 363^
0.8709 0.00236 36170.8717 0.00250 3617
7 0.8717 0.01358 368k0.8126 0.0021+8 3 6te
8 0.8126 -0.01191+ 360k0.881+1+ 0.00151 3653
O .8896 0.0021+8 3656
9 O .8896 0.0111+6 3695
0.81+15 0.00227 3660
0.81+27 0.00250 3661
10 0.81+27 0.001+16 3671
O.83I+O 0.0021+6 36650.831+2 0.00250 3665
11 O.83I+2 0.00786 36910.8067 0.00252 3671
12 0.8067 -O.OO65I 361*0
0.851!+ 0.00210 3671
0.8535 0.0021+9 3673
18
Table 1. Continued
Fueling(Cycle)
Fraction of Available Plutonium Recycled
Minimum Fraction Absorption
in Control Poison
End of Exposure Fissile Loading (kg)
13 0.8535 0.00628 36900.8338 0.002^7 36760 . ^ 0 0.00250 3676
Ik 0.83^0 O.OO267 367^0.8331 0.00250 3678
15 0.8331 0.00557 3693
0.8173 0.0021+9 3681
16 0.8173 -0.00258 3661*-
0.8^30 0.00238 3683
0.81*36 0.00250 3683
17 0.8^36 0.00^52 3692
0.8332 0.0021+9 3681*
18 0.8.332 0.00250 . 3686
19 0.8332 0.00^32 3695
0.8238 0.00251 3688
20 0.8238 -0.00039 3678
0.838U 0.002^5 3689
O .8387 0.00250 3689
21 O .8387 0.00361+ 3 69k0.8328 0.00250 3690
22 O .8328 0.002^8 3691
23 0.8328 0.003^5 3696
0.8280 0.00251 3692
2k 0.8280 0.0009^ 3687
0.8359 O.OOZkQ 3693
0.8360 0.00250 3693
25 0.8360 . 0.00309 3696
0.8330 0.00251 369^
19
specifies this management. Refer to Figure 1, the input sections 091
and 093 of the CITATION code report, and the printout of the input data
of these sections.
As an overview of the fuel management specifications for the problem,
the core was initially zoned and recycle feed handled such that three
fuel enrichments were used at each fueling. At each fueling, one-fourth
of the contents of an inner radial blanket zone was moved to an outer
radial blanket zone, and the replaced material removed and processed.
After one cycle delay, recycle feed was used to replace one-fourth of
the contents of the core, the replaced material removed and processed
along with that from the outer radial blanket. The axial blanket was
considered as an integral extension of the core fuel assemblies. With
this scheme, some material initially located in the inner radial blanket
remains there through the history up to the fifth fueling; and is finally
discharged from the reactor only at the ninth fueling; the bred plutonium
in these fuel assemblies is recycled to the core at the tenth fueling,
is finally discharged from it on the fourteenth fueling, and again re
cycled to the core at the fifteenth fueling. Excess bred plutonium is
not recycled.
Input section 093, card 2 instructs the code that additional data
on fraction of material recycled is to be included in the input (MAC13),
and each cycle is to be repeated a maximum of 5 times (MAC15) to attain
a specified minimum fraction loss to the search nuclide during each
cycle (MAC16), and that the recycle fractions are the parameters to be
adjusted to attain this desired condition (MACI7 ).
Cards 3, ^ and 5 give the desired minimum fraction loss to the search
nuclide as 0.0025 (FMC2), the convergence criteria to be satisfied for
the repeat cycle (FMC9)> and the fractions (of discharge material) that
are to be adjusted (FEM). Note that these numbers, FDM, are 1.0 for
this case since they will be adjusted by the code to attain the desired
condition. If the repeat cycle option were not being exercised, these
numbers could still be used to control the fraction of recycle material
that is recycled without iteration to a desired solution.
Cards 6 through 12 describe the fuel management to be carried out
for this entire history. The first number on these cards is a sequence
20
number. The second number, NFM2, identifies the fresh fuel feed stream
that is to be used prior to the availability of recycle material, fresh
fuel feed stream number 1 in all five specifications. Since there is 1
cycle delay in recycle (MST7, card 2 section 091), no recycle feed will
be available until the end of the second cycle and therefore the feed
to the zones to be refueled at the end of the first cycle will be the
initial loading of the zones as specified by NFFFS2=0 in the description
of fresh fuel feed stream number 1.
The next number, NFM3, identifies a fresh fuel feed stream to which
assignment of initial loading of material is to be made for suss balance
accounting. NFM}+ and NFM8 identify a makeup stream and a discharge stream
respectively for each of the seven separate specifications. A different
makeup stream is identified for each specification while material is
discharged from the reactor to discharge stream number 1 for all
specifications.
Consider the first specification, card 6. NFM^ identifies makeup
stream mueber 1 which is described in input section 091. Referring to
makeup stream 1, section 091, NFRFS3 identifies discharge stream number
1 as the source of recycle material, NFRFS6 identifies fresh fuel feed
stream dumber 2 as the source of fresh feed to be mixed with recycle feed,
and this fresh feed stream in turn specifies that the fresh feed concen
trations are specified since NFFFS2=1. (if NFFS2 had been 0, initial
loading concentration would have been used).
Continuing with makeup stream 1, QMTAR is a fraction applied to the
numbers FDM in addition to the calculated fraction determined by the
code when repeating cycles, as is done in this case. QJWTAR is used
primarily to distribute recycle feed to account for different zone
enrichments or volumes. Three different enrichments are used for this
problem in makeup stream 1, 2, and 3. Note the sum of ($4TAR for the
three streams is 1.0. DLTMR=0 specifies no decay, DPQR1=0 is recommended
at present since more work needs to be done in this area, and DPQJR2 gives
the gross fabrication loss, 0.996 for this stream. The recycle fractions
specified for this makeup stream 1 are applied prior to those given by
the fractions FDM and are primarily intended to be used to control what
21
material is to "be recycled -with entries of 1.0 or 0 0. For this stream
only the last four nuclides (l^, 15, 16, 17, see NIS1-NISA, cards 2J,
section 09l) will he recyc3.ed.
Makeup streams 2 and 3, identified for specifications 2 and 3, are
similar to makeup stream 1. Makeup streams ^ through 7, which are iden
tified to he used with specifications >-i through 7> specify no discharge
stream and therefore no recycle material will bo fed to the zones (NFM13+)
associated with these specifications. Also these makeup streams identify
fresh fuel feed stream 1 as source of fresh feed which will be the initial
concentrations (NFFFS2=0) of the nones involved.
The data given for discharge stream 1 is NFDFS1=1 which is a sequence
number, DLTM]}=200 wfcich instructs the code to decay all nuclides identified
on cards 3+ (only nuclide 16 for this case with a transition (decay)
constant of 1 .7 X lO-9) with At = 200 days, and a gross recovery fraction
DPQPe=0.995.
Back to cards 6+ of section O93, NFM12=:1, NFMll='l, and IJFM10=0, for
all seven specifications, say that all are to be applied to each cycle,
and they are to start from cycle number 1.
The numbers NFM13+ describe fuel management to be carried out for
each specification. With reference to Figure 1, WFM13 of the first
specification instructs the code to unload (to discharge stream l) and
refuel all zones of class 1, the two inner core zones 1 and 2. Since
there are four sub-zones specified (input section 012) for each of the
zones, 1 through 20, involved in the fuel management for this problem,
only one sub-zone will be unloaded and refueled, or moved from one zone
-go another, at each refueling (end of cycle), i.e., sub-zone 1,2,3, and lj,
at the end of cycles 1,2,3, and 1* respectively, and back to sub-zone 1
at the end of the fifth cycle, etc.
Specifications 2 through 6 instruct the code to unload and refuel
the appropriate sub-zone in all zones of class 2 through 6, respectively.
These include zones 3 through 12.
Specification 7 says that the appropriate sub-zones of zones 20, 19,
l8, and 17, are to be unloaded, material moved from zones 16 to 20, 15
to 19, 1^ t^ 18, and 12 to 17, and zones 16, 15, 1^, and 13 refueled.
22
Computer Edits
The edits of input data and results of calculations follow.
23
TABLE 2
ONE-DIMENSIONAL SLAB ( X ) . C J 0 1 -34X7 GROUPS , 2"3 POINTS • STREAM OF C I T A T I O N CASES ORNL 72 C J 0 1 -
0011 1
C J 0 1 -C J 0 1 -
1 1 1 1 15
C J C 1 -C J 0 1 -
100.0 0.0 001 C J 0 1 -003
1 1C J 0 1 -C J 0 1 -
o . o C J 0 1 -0 .0 1 .0 0 . 5 C J 0 1 -
004 C J 0 1 -8 1 0 . 0 8 10.0 8 1 0 .0 5 2 0 . 0 5 2 0 .0 C J O l -
005 C J 0 1 -1 1 1 2 2 C J 0 1 -
008 C J 0 1 -7 3 3 C J 0 1 -
1 1 2 .3 8 4 1 .198 - 0 2
9 .6 1 4 - 0 5 1.074 - 0 4 C J O l -C J 0 1 -
0 . C J 0 1 -1 2 1.221 1 .9 8 1 3 - 0 3
3 .5 4 6 - 0 36 .2 0 7 - 0 4 C J 0 1 -
C J 0 1 -C J 0 1 -
I 3 1 .227 1.6 554 - 0 3 1 .8232 .1 4 0
- 0 3- 0 2
C J 0 1 -C J 0 1 -C J O J -
1 4 1.2 25 2 , 1675 - 0 3 7 .8 2 7 - 0 4
3 .1 04 - 0 33 .6 4 3 - 0 2 1.821
C J 0 1 -- 0 4 C J 0 1 -
1.8 90 -0 4 C J 0 1 -] 5 1.1 45 6 .5 8 - 0 3 1 .0 03
1.049-0 2- 0 2 1.8 56
C J 0 1 -- 0 2 C J 0 1 -
2 .3 05 -0 3 C J 0 1 -1 6 0 .9 9 3 1 .1 1 3 8 - 0 2 1.7 29
1 .234- 0 2- 0 4 5 .9 4 6 - 0 2
CJ0 1- C J O J -
1.49 - 0 2 C JO 1-1 7 0 .9 1 7 5 2 .1 4 29 - 0 2 3.3 9 - 0 2 C J 0 1 -
4 .0 5 1 - 0 5 2 .257 - 0 2 4 .8 6 9 -0 2 C J 0 1- C J 0 1 -
? 1 1.8 391.562 - 0 2
5 .6 2 1 - 0 8 CJO 1- C J 0 1 -
0 . C J 0 1 -2 2 0 .9 4 8 2 .4 9 7 - 0 6
6 .3 6 9 - 0 3C J 0 1 -C J C 1 -C J 0 1 -
? 3 0 .9 3 2 9 2 .0 2 8 - 0 52 .9 8 6 - 0 2
C J C 1 - C J 0 1 - CJO 1-
2 4 0.9 432 6 .0 4 3 - 0 5 4 . 9 3 6 - 0 4 7 . 6 - 0 2 3 .6 1 6
C J 0 1 -- 0 4 C J 0 1 -
3 .7 5 7 -0 5 C J 0 1 -2 5 0.8 932 1 .172 - 0 4
7 .0 31 - 0 3 2 .8 9 3C J 0 1 -
- 0 2 C J 0 1 -3 .4 21 - 0 3 C J 0 1 -
? 6 0 .7 9 7 1 1.910 - 0 47 .0 6 6 - 0 5 6 .4 8 1 - 0 2
C J 0 1 - C JO 1 -
1.899 - 0 2 C J 0 1 -? 7 0.773 3 .4 1 9 - 0 4 C J 0 1 -
2 . 137 - 0 5 2 .2 0 9 - 0 2 5 .5 13 - 0 2 C J 0 1 -C J 0 1 -C J 0 1 -
0 .9 6 7 5 0 .0 3 2 5 C J 0 1 -C J 0 1 -C J 0 1 -
1 1 0 0 1 CORE C J 0 1 -
12345A789
10111213141516171819202122232425262728293031323334353637383940414243444546474849505152535455565758596061626364
2k
2 2 0 0 2 REFLF'CTDR C J O l -0 C J O l -
024 C J O l -1 0 . 0 C J 0 1 -
0^0 CJ01-C J 0 1 -
999 CJ01-UNE-DIMENSIONAL CYLINDER <R>. C J 0 1 -34X7 GROUPS» 238 P O IN TS . STREAM OF C I T A T I O N CASES ORNL 72 C J 0 1 -
001 C J 0 1 -1 1 C J 0 1 -
1 1 0 0 1 C J 0 1 -5 CJ0 1
1 0 0 .0 0 . 0 0 0 1 C J 0 1 -003 C J 0 1 -
2 1 C J 0 1 -0 . 0 C J O l -0 . 0 1 . 0 1 . 0 C J 0 1 -
004 C J 0 1 -8 2 2 . 3 9 8 2 2 .3 9 8 2 2 .3 9 5 2 0 .0 5 2 0 .0 C J 0 1 -
999 C J 0 1 -CINE-OIMENS IONAL SPHERE ( S ) . C J 0 1 -34X7 GROUPS» 238 P O IN T S . STREAM OF C I T A T I O N CASES ORNL 72 C J 0 1 -
003 C J 0 1 -3 1 C J 0 1 -
0 . 0 C J 0 1 -0 . 0 1 . 0 l . C C J 0 1 -
004 C J 0 1 -8 3 3 .3 3 3 8 3 3 .3 3 3 8 3 3 .3 3 3 5 2 0 . 0 5 2 0 . 0 C J C 1 -
999 C J 0 1 -
6 566676869707172737475767778798081828384858687888990919?9394
25
2~D PERTURBATION (OLD EXTERMINATOR CASE) C J 0 2 - 19X24X4 GROUP, 864 POINTS STREAM OF C I T A T I O N CASES ORNL 72 C J O ? - 2
0011 1 1
C J 0 2 -C J 0 2 -
34
1 1 1 1 1 1 C J 0 2 - 5100 C J 0 2 - 6
10.0 0 .0 0 1 C J 0 2 - 7003 C J 0 2 - 8
1 0 7 1 0 0 1 0 0 2 C J 0 2 - 90.0 001 0.0 0 0 1 C J 0 2 - 101 .0 E+30 - 4 . 0 C J 0 2 - 110 . 2 (D.2 0 . 2 0 .0 C J 0 2 - 12
004 C J 0 2 - 132 6 .0 2 4 . 0 3 1 2 .0 2 8 . 0 C J 0 2 - 144 8 . 0 7 1 4 . 0 13 2 5 . 0 C J 0 2 - 15
005 C J 0 2 - 163 ? 3 3 C J 0 2 - 171 2 1 3 C J 0 2 - 181 1 1 3 C J 0 2 - 19
008 C J 0 2 - 204 3 3 C J 0 2 - 21
1 1 0 .5 0002 80.0 11
0 .0 2 80 .0 0 0 5
0 . 0 0 40.0 0 0 2 5
C J 0 2 - C J 0 2 -
2223
1 2 0 .5 0002 8 0 .0 3 6 0 .0 0 8 C J 0 2 - 240.0 0 0 2 0 . 0 1 6 0 .0 0 0 5 C J 0 2 - 25
1 3 0 .5 0002 5 0 . 0 6 0 .0 1 C J 0 2 - 260.0 0 0 1 0 .0 0 0 2 0 .0 2 2 C J 0 2 - 27
1 4 0.5 0002 8 0 .0 9 0 .0 4 C J 0 2 - 280 . 0 C J 0 2 - 29
2 4 1 . 0 0.0001 C J 0 2 — 300 . 0 C J 0 2 - 31
3 1 0.9990020 .0 0 0 5
0.0001250 . 0 0 0 3 0 .0 0 0 2
C J 0 2 -C J 0 2 -
3233
3 2 0.999002 0 .0 0 0 2 3 C J 0 2 - 340 .0 0 0 4 0 .0 0 1 3 0 .0 0 0 4 C J 0 2 - 35
3 3 0.9 9900 2 0 .0 0 3 0 5 C J 0 2 - 360 .0 0 0 3 0 .0 0 0 6 0 .0 0 2 1 C J 0 2 - 37
3 4 0.9 9900 2 0 .0 0 4 0 6 C J 0 2 - 380.0 0 0 2 0 .0 0 0 8 0 . 0 0 1 C J 0 2 - 39
0 C J 0 2 - 400 . 6 0 . 2 0 . 1 O • N* C J 0 2 - 41
024 C J 0 2 - 421 0 .0 0 1 C J 0 2 - 43
040 C J 0 2 -C J 0 2 -
4445
999 C J 0 2 - 462 - 0 C A S E P E R T U R B E D T O C H E C K P E R T U R B A T I O N R E S U L T * 0 ( 1 * 1 1 C H A N G E D - . 0 5 C J 0 2 - 4 7
9 X 2 4 X 4 G R O U P , 8 6 4 P O I N T S 001
1100 10.0
0 0 8 4 3
1
1 1 1
0.001
1 0 . 4 5 0 0 2 8 0.011
0 .2
0 . 0 2 80 . 0 0 0 5
0 . 1
S T R E A M OF C I T A T I O N C A S E S O R N L 7 2
1 1
5
0 . 0 0 40 . 0 0 0 2 5
0 .10.6 0 2 4
1 0.001 9 9 9
2 - 0 C A S E P E R T U R B E D T O C H E C K P E R T U R B A T I O N R E S U L T , D f l , l ) C H A N G E D - . 2 5 9 X 2 4 X 4 f c R O U P , 8 6 4 P O I N T S S T R E A M U F C I T A T I O N C A S E S O R N L 7 2
C J 0 2 - 4 8 C J 0 2 - 4 9 C J 0 2 - 5 0 C J 0 2 - 5 1 C J 0 2 - 5 2 C J 0 2 - 5 3 C J 0 2 - 5 4 C J 0 2 - 5 5 C J 0 2 - 5 6 C J 0 2 - 5 7 C J 0 2 - 5 8 C J 0 2 - 5 9 C J 0 2 - 6 0 C J 0 2 - 6 1 C J 0 2 - 6 2 C J 0 3 - 1C J 0 3 - 2
26
008 4 3
1
0 . 6024
1 0.001 999
1 0 . 2 5 0 0 1 4 0.011
0 . 2
0 o0280.0 0 0 5
0. 1
0 .0 0 40 .0 0 0 2 5
0. 1
C J O B - 3 C J 0 3 - 4C J 0 3 - C J 0 3 - C J 0 3 - C J 0 3 - CJ03- C J 0 3 - 10 C J 0 3 - 11
5678 9
27
2 - D FIXED SOURCE PROBLEM ( X , Y - NO F I S S I O N SOURCE, AFTER KAPLAN) C J 0 3 - 1239X41X1 GROUP? 1599 POINTS STREAM OF C I T A T I O N CASES ORNL 72 C J 0 3 - 13
001 C J 0 3 - 145 1 C J 0 3 - 15
1 1 1 1 1 1 C J 0 3 - 1650 C J 0 3 - 17
C J 0 3 - 18003
6 i 1 1 1C J 0 3 - 19 C J 0 3 - 20 C J 0 3 - 21 C J 0 3 - 22
004 C J 0 3 - 232 0 .90 88 15 7 .7 7 6 1 5 1.6802 15 7.7 7 6 1 2 0 .9 0 88 C J 0 3 - 24
17 8 .8 1 3 8 4 1 .4 2 2 4 2 0 .2 8 0 9 15 6 . 8 2 9 2 3 1 .7 0 3 7 C J O B - 25005 C J 0 3 - 26
5 1 5 2 5 C J 0 3 - 275 5 5 5 5 C J 0 3 - 285 5 5 3 5 C J 0 3 - 295 4 5 3 5 C J 0 3 - 305 5 5 3 5 C J 0 3 - 31
008 C J 0 3 - 321 0 0 C J 0 3 - 33
1 1 2 .0 9 5 0 0 6 . 4 2 5 6 0 - 2 C J 0 3 - 340 . 0 C J 0 3 - 35
2 1 2 .0 9 5 00 6 . 4 2 5 6 0 - 2 C J 0 3 - 360 . 0 C J 0 3 - 37
3 1 2 .0 9 5 0 0 6 . 4 2 5 6 0 - 2 C J 0 3 - 380 . 0 C J 0 3 - 39
4 1 2 .2 0 0 7 9 6 . 2 1 5 8 0 - 2 C J 0 3 - 400 . 0 C J 0 3 - 41
5 1 2 .2 3 8 1 3 4 . 9 5 9 1 0 - 2 C J 0 3 - 420 . 0 C J 0 3 - 43
0 C J 0 3 - 440 . 0 C J 0 3 - 45
012 C J 0 3 - 461 1 BLANKET 1 C J 0 3 - 472 2 BLANKET 2 C J 0 3 - 483 3 BLANKET 3 C J 0 3 - 494 4 SEED C J 0 3 - 505 5 MOD-STR C J 0 3 - 510 C J 0 3 - 52
024 C J 0 3 - 531 C J 0 3 - 54
026 C J 0 3 - 55- 1 1 C J 0 3 - 56
1 . 0 C J 0 3 - 571 2 . 1 4 2 3 1 - 3 2 2 . 1 5 0 2 4 - 3 3 2 . 1 7 7 2 9 - 3 4 1 . 0 4 8 0 8 - 2 C J 0 3 - 58
999 C J 0 3 - 59
28
2 - D FIXED SOURCE PROBLEM WITH F I S S I O N SOURCE C J 0 4 - 120X20X1 GROUP* 400 P OIN TS STREAM OF C I T A T I O N CASES ORNL 72 C J 0 4 - 2
001 C J 0 4 - 3“ 5 1 C J 0 4 - 4
1 0 1 1 1 1 0 0 0 1 0 C J 0 4 - 550 C J 0 4 - 6
1 0 .0 1 . 0 - 3 0 C J 0 4 - 7003 C J 0 4 - 8
6 C J 0 4 - 9C J 0 4 - 10
1 .0 1 .0 1 . 0 C J 0 4 - 11004 C J 0 4 - 12
8 4 . 0 12 6 . 0 C J 0 4 - 1312 6 . 0 8 4 . 0 C J 0 4 - 14
005 C J 0 4 - 151 1 C J 0 4 - 162 1 C J 0 4 - 17
008 C J 0 4 - 181 C J 0 4 - 19
1 12 .2 0 0 2 2 0 . 0 6 2 2 0 .2 1 6 C J 0 4 - 200 . 0 C J 0 4 - 21
2 1 2 .2 0 0 2 2 0 .1 3 6 5 0 .0 3 6 2 8 2 2 C J 0 4 - 220 . 0 C J 0 4 - 23
0 C J 0 4 - 241 . 0 C J 0 4 - 25012 C J 0 4 - 26
1 1 MATERIAL 1 C J 0 4 - 272 2 MATERIA L Z C J 0 4 - 28
C J 0 4 - 29024 C J 0 4 - 30
1 C J 0 4 - 31026 C J 0 4 - 32
0 0 C J 0 4 - 331 . 0 C J 0 4 - 34
1 20 1 12 1 . 0 C J 0 4 - 359 20 13 20 1 . 0 C J 0 4 - 360 C J 0 4 - 37
999 C J 0 4 - 38
29
2 - 0 SEARCH ON ABSORBER, BARE SLAB WITH UPSCATTER♦ ANS BENCHMARK PROBLEM C J 0 5 - 22X4X7 GROUPS, 616 POINTS STREAM OF C I T A T I O N CASES ORNL 72 C J 0 5 -
001- 0 1 1 1
C J 0 5 -C J 0 5 -
1 1 0 0 1 05
C J 0 5 -C J 0 5 -
1 0 . 0 0 .0 0 1 C J 0 5 -003 C J 0 5 -
1 0 0 0 6 0 0 0 0 0 1 0 0 1 0 0 0 0 0 0 0 0 0 O C J O S - C JO 5 -
1 . 0 E+30 C J 0 5 -004 C J 0 5 -
22 6 7 .5 C J 0 5 -4 1 3 . 5 C J 0 5 -
00 5 C J 0 5 -1 C J 0 5 -
008 C J 0 5 -7 4 2 C J 0 5 -
1 1 1 . 60 .0 1 5
0 .0 10 . 0 1
0 . 0 20 . 0 1
0 . 0 10 . 0 0 5
C J 0 5 -C J 0 5 -C J 0 5 -
1 2 1 . 4 0 . 0 20 . 0 2
0 . 0 10 . 0 2
0 . 0 20 . 0 1 0 .0 1
C J 0 5 -C J 0 5 -
0 C J 0 5 -1 3 1 .2 0 . 0 3 0 . 0 2
0 . 0 20 . 0 3
0 . 0 2 0 . 0 1C J 0 5 -C J 0 5 -
0 . 0 1 C J 0 5 -1 4 1 . 0 0 . 1 0 0 . 0 4 0 . 10
0 . 0 3 0 . 0 2C J 0 5 -C J 0 5 -
0 .0 1 C J 0 5 -1 5 0 . 8 0 .0 5 0 . 1 0 0 . 0 5
0 . 0 5C J 0 5 -C J 0 5 -
0 . 0 3 C J 0 5 -1 6 0 . 6 0 . 0 7 0 . 1 2 0 . 0 7
0 . 0 2C J 0 5 -C J 0 5 -
0 .0 8 C J 0 5 -1 7 0 . 4 0 .0 9 0 . 1 5 0 . 0 9
0 . 0 2 0 . 0 6C J 0 5 -C J 0 5 -
0 C J 0 5 -0 C J 0 5 -
0 . 9 0 . 0 9 0 .0 1 C J 0 5 -C J 0 5 -
024 C J 0 5 -1 C J 0 5 -
040 C J 0 5 -C J 0 5 -
999 C J 0 5 -
123456789
10111213141516171819202122232425262728293C3132333435363738394041424344454647
30
2 - D FAST REACTOR DIMENSION SEARCH C J 0 6 -27X18X5 GROUP, 2430 POIN TS STREAM OF C I T A T I O N CASES ORNL 72 C J 0 6 -
OOO C J 0 6 -8 C J 0 6 -
HOMOGENEOUS DESIGN 2 REACTOR C J 0 6 -1 15 5 4 0 0 C J 0 6 -
7 .5 5 0 3 7 E -0 1 2 .38025ft - 0 1 6 . 9 3 8 0 0 E - 0 3 0 . 0 0 . 0 C J 0 6 -1 .4 9 1 8 2 E 07 8 .2 0 8 5 0 E 05 6 . 7 3 7 9 5 E 04 9 .Z 1 8 8 2 E 03 7 .4 8 5 1 9 E 02 C J 0 6 -3 .4 9 9 3 8 E 06 2 .3 5 1 7 7 E 05 2 .4 7 8 7 5 E 04 2 .6 1 2 5 9 E 03 2 .7 3 5 9 1 E - ■01 C J 0 6 -3 . 8 7 6 0 8 E ' - 0 4 1 .1 2193 E - 0 3 3 . 0 8 1 6 3 E - 0 3 9 . 1 4 2 6 6 E - •03 2 . 3 9 3 9 7 E - •02 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
©•oC J 0 6 -
0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 o • o
o•o
C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -
10 1922351 0 0 0 URANIUM-235 C J 0 6 -2 . 3 3 0 2 5 E 02 0 . 0 3 . 1 4 8 1 0 E - 1 1 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 , 0 1 .2 5 0 0 0 E 0 1 C J 0 6 -1 .2 5 0 0 0 E 01 0 . 0 0 . 0 6 ,8 9 0 0 0 E 02 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -1 .3 4 3 9 4 E 00 1 .2 7641 E 00 4 . 7 6 0 5 0 E 00 2 . 6 6 7 8 6 E 00 2 . 1 2 5 4 5 E 00 C J 0 6 -1 . 7 1 8 1 IE 00 1 .4 2 2 7 7 E 00 8 .2 2 2 5 5 E ‘00 2 .4 5 7 8 8 E 00 1.83163 E 00 C J 0 6 -3 .2 2 9 8 4 E 00 2 .3 9 7 5 4 E 00 1.3.5953E 01 2 . 4 3 3 3 8 E 00 3 .2 5 9 9 4 E 00 C J 0 6 -7 .6 9 0 4 0 E 00 5 . 3 4 9 6 6 E 00 1.9 1 4 3 2 E 01 2 . 4 3 0 3 8 E 00 7 .7 0 9 5 4 E 00 C J 0 6 -2 . 0 4 4 7 7 E 01 1 .4 3335 E 01 3 . 1 8 0 2 3 E 01 2 .4 3 0 0 7 E 00 2 .0 4 4 7 7 E 01 C J 0 6 -4 .8 5 6 9 7 E 00 7 . 7 4 9 8 1 E - 0 1 6 . 2 6 2 0 8 E - 0 3 0 . 0 0 . 0 0 . 0 C J 0 6 -7 . 9 8 3 6 7 E 00 1 .1 2862 E -0 1 6 . 0 1 9 3 8 E -0 4 0 . 0 0 . 0 0 . 0 C J 0 6 -1 .0 6 1 9 8 E 01 3 . 0 0 6 1 5 E - 0 2 2 . 0 7 6 5 5 E -0 5 0 . 0 0 . 0 0 . 0 C J 0 6 -1•135 63 E 01 1 .9 1 1 2 5 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -1 .1 7 2 9 1 E 01 C J 0 6 -
12 1922380 0 0 0 URANIUM-238- -RESONANCE C J 0 6 -2 . 3 6 0 0 6E 02 0 . 0 3 . 1 6 2 5 O E - 1 1 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 9 . 0 G 0 0 0 E 0 0 C J 0 6 -9 . 0 0 0 0 0 E 00 0 . 0 0 . 0 2 .7 1 0 0 0 E 00 o . o 0 . 0 C J 0 6 -0 . 0 0 , 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0*0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -4 .1 9 1 7 8 E . -0 1 3 . 3 4 6 0 2 E - 0 1 4 .8 4 6 7 6 E 00 2 .7 8 6 5 2 E 00 2 .2 8 2 7 4 E 00 C J 0 6 -1 . 7 0 4 5 5 E - 0 1 2 .3 7 6 5 2 E - 0 4 8 . 5 7 1 0 4 E 00 2 . 4 6 6 4 4 E 00 3 . 0 6 7 5 1 E - 0 1 C J 0 6 -4 . 8 0 4 5 3 E - 0 1 0 . 0 1 .3 4 4 9 7 E 01 0 . 0 5 .2 1 9 5 5 E - -01 C J 0 6 -9 . 7 3 5 6 5 0 - 0 1 0 . 0 1 . 7 6 8 1 5 E 01 0 . 0 9 . 9 2 5 5 4 E -0 1 C J 0 6 -1 . 3 8 1 5 4 E 00 0 . 0 1 .8 9 0 2 3 E 01 0 . 0 1 .3 8158 E 00 C J 0 6 —4 . 9 8 8 9 1 E 00 1 .8 1843 E 00 4 . 4 7019 E—02 2 . 0 6 2 6 6 E - •04 0 . 0 0 . 0 C J0 6 —1 .0 0 2 5 2 E 01 1 .3 5 7 5 7 E - 0 1 5 . 15200E—04 0 . 0 0 . 0 0 . 0 C J 0 6 —1 . 3 2 5 6 7 E 01 4 .1 1 0 7 9 E - 0 2 3 . 8 ^ 7 1 5 E - 0 4 0 . 0 0 . 0 0 . 0 C J 0 6 -1 .6 9 8 0 6 E 01 1 .8 9 7 4 4 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -1 .8 3 8 3 8 E 01 C J 0 6 -
14 1.942390 0 0 0 P LUTONIU M-239-RESONANCE C J 0 6 -2 . 3 6 9 9 9 E 02 0 . 0 3 . 2 5 8 6 0 E - 1 1 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 1 . 2 0 000E 0 1 C J 0 6 -1 . 2 0 0 0 0 E 01 0 . 0 0 . 0 1 . 0 2 6 0 0 E 03 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 —0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -0 . 0 0 . 0 0 . 0 0 . 0 o . o o . o C J 0 6 -
12
4
67fl9
101 IIP1314lc16171819202122232425262728293031323334353637383940414243444546474849505152535455565758596061626364
31
0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 650 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 660 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 671 .9 0 1 7 7 E 00 1.8 8 3 0 7 E 00 4 . 9 5 4 3 1 E 00 3 .1 5 9 67E 00 2 .6 1 3 7 7 E 00 C J 0 6 - 681 .7 1497 E 00 1 . 5 4 4 6 3 E 00 8 .7 1 8 1 8 E 00 2 .9 0 8 9 3 E 00 1.8 3 4 8 6 E 00 C J 0 6 - 692 . 3 4 1 2 1 E 00 1.7 9 3 6 5 E 00 1 .4 1793E 01 2 .8 7 4 1 3 E 00 2 . 9 9 5 1 4 E 00 C J 0 6 - 705 .2 7 9 3 0 E 00 3 . 5 2 0 4 7 E 00 1.94812 E 01 2 . 8 7 0 4 9 E 00 7 .1 8 9 9 1 E 00 C J 0 6 - 711 . 4 4 8 2 1 E 01 9 . 3 7 6 2 9 E 00 3 . 2 7 1 9 6 E 01 2 .8 7 0 0 6 E 00 2 .0 3 0 5 8 E 01 C J 0 6 - 724* 75510E 00 6 .9 7 7 4 4 E - 0 1 1 .4 0 3 8 9 E - ■02 0 . 0 0 . 0 0 . 0 C J 0 6 - 738 . 6 6 0 60E 00 5 .9 3 8 3 3 E - 0 2 1 . 3 9 3 6 5 E-•04 0 . 0 0 . 0 0 . 0 C J 0 6 - 741 .1 5208 E 01 5 .9 9 6 5 4 E - -0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 751 . 2 2 8 1 1 E 01 2 .2 4 7 6 4 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 761.3 2171 E 01 C J 0 6 - 77
15 1942400 0 0 0 P LU TONIUM -2 40-R E S ONANCE C J 0 6 - 782 .3 7 9 9 0 E 02 0 . 0 3 . 2 8 270E-■11 0 . 0 0 . 0 0 . 0 C J 0 6 - 790 . 0 0 . 0 0 . 0 0 . 0 0 . 0 9 eOoOOOE 0 0 C J 0 6 - 809 .0 0 0 0 0 E 00 0 . 0 0 . 0 2 .9 5 0 0 0 E 02 0 . 0 0 . 0 C J 0 6 - 810 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 820 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 830 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 840 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 850 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 860 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 870 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 CJ06 — 881.63837 E 00 1 . 5 4 3 4 6 E 00 5 .0 5 4 4 7 E 00 3 .1 4 6 5 3 E 00 2 .5 7 0 0 8 E 00 C J 0 6 - 894 . 4 2 7 2 2 E - 0 1 2 . 3 2 7 8 4 E -0 1 8 . 6 0 4 6 7 E 00 2 .9 3 5 9 4 E 00 5 . 4 0 2 0 5 E — 01 C J 0 6 - 906 . 8 3 4 9 4 E - 0 1 l c 0 0 8 2 3 E -0 1 1 .3 7 1 4 2 E 01 2 .8 7 4 2 6 E 00 7# 2 1 2 2 9 E - 0 1 C J 0 6 - 911 .8 4 8 1 9 E 00 8 •2‘!>824E—02 1 .8 8 8 1 7 E 01 2 . 8 7 0 6 5 E 00 1 .8 8 9 5 3 E 00 C J 0 6 - 9?5 .5 9 3 6 7 E 00 5 .7 8 6 9 0 E - -0 2 2 .4 1 8 4 9 E 01 2 . 8 7 0 0 7 E 00 5 .5 9 7 2 9 E 00 C J 0 6 - 9 34 . 9 4 4 1 1 E 00 9 .1 5 2 2 5 E -0 1 1 . 6 1 7 9 2 E - ■02 1 . 0 9 1 3 2 E - 0 4 0 . 0 0 . 0 CJOA— 941.00410 E 01 9 . 7 4 1 5 9 E - 0 2 4 . 50826E—05 0 . 0 0 . 0 0 . 0 C J 0 6 - 9 51 . 3 3 2 4 2 E 01 3 .6 5 7 1 2 E ' -0 2 1*64276E-■05 0 . 0 0 . 0 0 . 0 C J 0 6 - 961.6 9 6 7 0 E 01 3 .2 3 7 7 6 E - - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 971 .9 2 1 1 4 E 01 C J 0 6 - 98
16 1942410 0 0 0 PLUTO NIUM -24 1 C J 0 6 - 992 . 3 8 9 7 8 E 02 0 . 0 3 . 30510 E--11 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 00 . 0 0 . 0 0 . 0 0 . 0 0 . 0 1 .2 0 0 0 0 E 0 1 C J 0 6 - 1 0 11 . 2 0 0 0 0 E 01 0 . 0 0 . 0 1 . 4 0 0 0 0 E 03 0 . 0 0 . 0 C J 0 6 — 1020 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C JO 6— 1030 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 — 1050 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 0 91 .7 3 0 3 4 E 00 1 .7 0 3 6 5 E 00 5 . 1 0 4 2 3 E 00 3 .2 5 6 9 4 E 00 2 . 9 6 7 4 9 E 00 C J 0 6 — 1102 .0 8 7 2 6 E 00 1 .8 6 9 9 6 E 00 8 . 6 4 385E 00 3 . 0 0 5 6 2 E 00 2 .4 1 1 7 8 E 00 C J 0 6 - 1 1 13 . 6 4 3 2 7 E 00 3 .0 3 6 8 6 E 00 1 .2 6 9 6 3 E 01 2 .9 7 3 2 8 E 00 3 . 6 8 6 0 9 E 00 C J 0 6 - 1 1 28 .3 2 2 9 4 E 00 6 . 6 5 3 9 5 E 00 1 .9 7 646E 01 2 . 9 6 9 4 9 E 00 8 . 3 4 3 7 IE 00 C J 0 6 - 1 1 32 . 5 5 7 2 8 E 01 1 .9 9 5 8 6 E 01 3 . 7 6 7 0 9 E 01 2 .9 6 9 0 6 E 00 2 .5 5 7 2 8 E 01 C J 0 6 — 1144 .5 2 9 6 7 E 00 1 .1 6 5 4 5 E 00 7 . 1 2 2 9 5 E -0 2 2 . 5 5 0 6 6 E - 0 4 0 . 0 0 . 0 C J 0 6 - 1 1 57 . 8 7 3 8 2 E 00 3 .1 8 8 0 4 E ' -0 1 5 . 6 5 7 0 0 E-■03 0 . 0 0 . 0 0 . 0 C J 06— 1169 .1 1 3 9 9 E 00 4 . 1 4 1 5 3 E - 0 2 1 . 3 9 103E- 03 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 1 71 .1 2 7 1 9 E 01 2 .0 7 7 5 0 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 1 81 .2 9 9 9 0 E 01 C J 0 6 - 1 1 9
17 1942420 0 0 0 P LU TO N IU M -2 4 2 -R E S ONANC E C J 0 6 - 1 2 02 . 4 0 1 4 5 E 02 0 . 0 3 . 2 7 6 2 0 E - ■11 0 . 0 0 . 0 0 . 0 C J O 6— 1210 . 0 0 . 0 0 . 0 0 . 0 0 . 0
UJooooo• OOCJO6 — 1229 . 0 0 0 0 0 E 00 0 . 0 0 . 0 3 .O C 0 0 0 E 01 0 . 0 0 . 0 C J O 6— 1230 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 2 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 2 50 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 2 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 2 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 06— 1280 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 2 90 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 3 0
32
1.49519E 00 1 .4 5354 E 00 4 . 4 9 3 7 8 E 00 3 . 12280E 00 2 . 11010E 00 C J 0 6 - I 3 12 . 7 5 6 7 0 E - -01 1 . 3 9 8 2 3 E - 0 1 7 .7 2116 E 00 2 .8 8 5 6 3 6 00 4 . 0 4 8 5 5 E — 01 C J 0 6 - 1 3 24 . 9 7 9 4 0 E - -01 4 . 6 3 2 3 2 E - 0 2 1.41695E 01 2 .8 1 2 2 9 E 00 5 .4 3 9 0 8 E -0 1 C J 0 6 - 1 3 31 .5 3 5 0 6 E 00 0 . 0 2 .0 9 3 3 8 E 01 0 . 0 1 .5 7 0 3 0 E 00 C J 0 6 - 1 3 45 .9 0 0 1 IE 00 0 . 0 2 .8 6 6 1 2 E 01 0 . 0 5.9 0016 E 00 C J 0 6 - 1 3 55 .0 5 1 7 0 E 00 6 . 0 3 7 6 5 E -0 1 1 . 0 9 2 2 4 E-■02 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 3 69 .3 5 6 9 4 E 00 1 .2 9 1 5 8 E —01 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 3 71 .4 3 3 5 8 E 01 4 . 5 8 9 5 I E —02 6 . 6 24 37 E-•05 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 3 81.9 3521 E 01 3 . 5 2 2 3 5 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 3 92 .4 3 1 7 6 E 01 C J 0 6 - 1 4 0
23 180160 0 0 0 OXYGEN-16 G J 0 6 -1 4 11 . 5 8620E 01 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 20 . 0 0 . 0 0 . 0 0 . 0 0 . 0 3 . 8 0 0 0 0 E OOCJOft-1433 .8 0 0 0 0 E 00 0 . 0 0 . 0 2 . 0 0 0 0 0 E -0 4 0 . 0 0 . 0 C J 0 6 - 1 4 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 50 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 4 90 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 5 00 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 5 16 . 0 5 8 6 6 E - 0 3 0 . 0 2 .0 0 1 4 2 E 00 0 . 0 4 , 33363E-01 C J 0 6 - 1 5 20 . 0 0 . 0 3 .5 3 8 1 9 E 00 0 . 0 1 . 7 5 9 4 5 E - 0 1 C J 0 6 - 1 5 30 . 0 0 . 0 3 . 5 3090E 00 0 . 0 1 . 3 0 4 2 8 E -0 1 C J 0 6 - 1 5 40 . 0 0 . 0 3 .5 8648 E 00 0 . 0 8.49 2 7 6 E - 0 2 C J 0 6 - 1 5 54 . 3 8 8 4 9 E - 1 6 0 . 0 3 .8 0 2 4 4 E 00 0 . 0 4 . 7 6 8 3 7 E -0 6 CJI0 6 -1 5 62 .1 6 6 4 7 E 00 4 . 2 7 2 8 7 E —01 1 . 12223E—07 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 5 73 . 6 4 7 6 0 E 00 1 .7 5 9 3 3 E - 0 1 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -1 5 83 .4 6 3 1 2 E 00 U 3 0 4 2 3 E - 0 1 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 5 93 .56 2886 00 8 . 4 9 2 5 9 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 6 03 .6 7 7 5 9 E 00 C J 0 6 - 161
25 1110230 0 0 0 SODIUM-23-RESONANCE (CO C J 0 6 - 1 6 22 .2 7 8 6 0 E 01 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J06.-1630 . 0 0 . 0 0 . 0 0 . 0 0 . 0 3 . 2 0 0 0 0 E C 0 C J 0 6 -1 6 43 . 2 0 0 0 0 E 00 0 . 0 0 . 0 5 . 0 5 0 0 0 E - •01 0 . 0 0 . 0 • C J 0 6 - 1 6 50 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 6 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 6 70 , 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 6 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1690 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -1 7 Q0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 7 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 7 21 . 7 8 8 0 1 E - 0 3 1 . 5 4 X 6 3 E - 0 6 2 .0 3 6 9 7 E 00 2 . 0 0 0 0 0 E 00 4 . 2 0 6 4 4 E - 0 1 C J 0 6 - 1 7 35 . 1 4 6 4 9 E - 0 4 0 . 0 3 . 5 3 8 7 5 E 00 0 . 0 U 3 2 9 7 2 E - 0 1 C J 0 6 - 1 7 41 . 0 9 4 2 0 E - 0 3 0 . 0 4 . 9 7 0 7 IE 00 0 . 0 1.4-2107E—01 C J 0 6 - 1 7 51 .2 0 7 1 1 £•-0 2 0 . 0 1 .1 5 4 0 6 E 01 0 . 0 5 .6 8 5 4 2 E -0 2 C J 0 6 - 1 7 65 . 8 1 6 2 2 E - 0 3 0 . 0 3 . 1 9 254E 00 0 . 0 5 . 8 1 7 4 1 E - 0 3 C J 0 6 - 1 7 72 . 6 2 2 2 1 E 00 4 . 1 8 6 4 8 E - 0 1 1 . 4 5 2 6 0 E -0 4 0 . 0 0 . 0 0*0 C J 0 6 - 1 7 83 .7 4 3 6 0 E 00 1 . 3 2 4 4 3 E - 0 1 0 . 0 0 . 0 0 . 0 0 . 0 C J O 6— 1794 .8 5 7 2 8 E 00 1 .4 1 4 8 4 E - 0 1 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 8 01 .6 0931 E 01 5 . 4 4 9 7 4 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 8 13 .0 5 4 2 3 E 00 C J 0 6 - 1 8 2
31 1240000 0 0 0 CHROMIUM C J O 6 - 1 8 35 . 2 0 1 0 0 E 01 0 . 0 0 . 0 0 . 0 0 . 0 0*0 C J 0 6 - 1 3 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 4 . 3 0 0 0 0 E OOCJO6- I 854 . 3 0 0 0 0 E 00 0 . 0 0 . 0 3 . 1 0 0 0 0 E 00 0 . 0 0 . 0 C J 0 6 - 1 8 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 8 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 » 0 C J 0 6 - 1 8 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J O S - 1890 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 9 00 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 9 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 9 20 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 1 9 33 . 4 8 2 5 9 E - 0 3 0 . 0 1 .8 9 5 96E 00 0 . 0 2 . 5 0 6 3 7 E - 0 1 C J 0 6 - 1 9 44 . 5 9 4 6 9 E - 0 3 0 . 0 2 . 8 4 7 7 0 E 00 0 . 0 4 .3 5 8 2 0 E —02 C J 0 6 - 1 9 57 .5 4 8 5 5 E - -0 3 0 . 0 4 .0 9 9 5 4 E 00 0 . 0 1 . >.698lf— 0 i C J 0 6 - 1 9 6
33
1 . 3 7 4 7 0 E - 0 1 0 . 0 1.25 856E 01 0 . 0 1 . 6 8 7 2 4 E - 0 1 C J 0 6 - 19 71 . 2 5 7 8 2 E - 0 1 0 . 0 4 , 4 8 5 0 6 E 00 0 . 0 1. 25800 E -0 1 C J 0 6 - 1 9 82.6 5 4 6 1 E 00 2 . 4 0 5 1 8 E - 0 1 6 . 12858E--0 3 4 . 7 8 3 0 8 E - 0 4 2 . 7 8 5 9 6 E -0 5 0 . 0 C J 0 6 - 1 9 93 .6 7 2 3 8 E 00 3 . 8 9 8 3 9 E - 0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 0 04 .2 6 8 3 6 E 00 1 .0 9 4 2 9 E —01 0. 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 0 11 .2 4 3 1 9 E 01 3 . 1 2 2 9 0 E -0 2 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 0 24 .2 9 6 3 4 E 00 C J 0 6 - 2 0 3
32 1250551 0 0 0 MANGANESE-55 C J 0 6 - 2 0 45.4 4 6 6 0 E 01 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 0 50 . 0 0 . 0 0 . 0 0 . 0 0 . 0 2 .30000E OOCJ0 6 -2 0 62 .3 0 0 0 0 E 00 0 . 0 0 . 0 1 . 3 2 0 0 0 E 01 0 » 0 0 . 0 C J 0 6 - 2 0 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 C J 0 6 - 2 0 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C JO 6 -2 0 90 . 0 0 . 0 0 . 0 0 . 0 O.'O 0 . 0 C J 0 6 -2 1 00 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 1 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 1 20 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 1 30 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -2 1 44 . 4 4 1 7 2 E - 0 3 1 . 0 7 3 1 0 E - 0 4 2.5 9165 E 00 2 . OOOOOE 00 4 . 5 0 5 9 3 E - 0 1 C J 0 6 - 2 1 51 . 1 3 4 8 9 E - 0 2 0 . 0 5 .2 3 5 5 3 E 00 0 . 0 2 . 0 2 4 5 7 E - 0 1 CJ 0 6 - ? 1.45 . 4 4 8 2 1 E - 0 2 0 . 0 1 .4 5 6 4 IE 01 0 . 0 4 . 8 7 3 2 4 E - 0 1 C J 0 6 - 2 1 73 .6 5 2 8 7 E - 0 1 0 . 0 6 .2 3 1 1 6 E 01 0 . 0 4 . 6 6 4 6 1 E -0 1 C J 0 6 - 2 1 83.2 0907 E 00 0 . 0 1 .0 0 266E 02 0 . 0 3 .2 0 9 4 1 E 00 C J 0 6 - 2 1 92 .9 7 4 7 2 E 00 4 .2 6 3 6 8 E -0 1 1.91190E- -02 5 . 5 2 6 4 7 E -0 4 0 . 0 0 . 0 C J 0 6 - 2 2 05.4 3689 E 00 1 . 8 5 1 7 8 E - 0 1 5 .9 1 8 1 7 E —03 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 2 11 .3 9 6 7 5 E 01 4 . 3 2 8 4 2 E —01 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 2 27 .8 1 7 0 1 E 01 1 . 0 1 1 9 8 E - 0 1 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 2 31 . 4 6 8 2 0 E 02 C J 0 6 - 2 2 4
33 1260000 0 0 5 IRON C J 0 6 — 2255 .5 8 4 5 0 E 01 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 2 60 . 0 0 . 0 0 . 0 0 . 0 0 . 0 i . H O O O E 0 1 C J 0 6 - 2 2 71 .1 1 0 0 0 E 01 0 . 0 0 . 0 2 . 5 3 0 0 0 E 00 0 . 0 0 . 0 C J 0 6 - 2 2 80 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 2 90 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 -2 3 00 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 3 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 3 20 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 3 30 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 CJ 0 6 -2 3 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2352 . 5 1 9 8 5 E - 0 3 0 . 0 2 .1 6 8 0 9 E 00 0 . 0 0 . 1 C J 0 6 - 2 3 65 . 2 5 2 5 0 E - 0 3 0 . 0 3 . 4 8 269E 00 0 . 0 C J 0 6 - 2 3 71 . 9 4 6 3 8 E - 0 2 0 . 0 6 .5 6 6 1 2 E 00 0 . 0 C J 0 6 - 2 3 85 . 0 7 4 9 1 E - 0 2 0 . 0 9 . 0 3 109E 00 0 . 0 C J 0 6 - 2392 . 0 5 6 8 3 E—02 0 . 0 1.0 5557 E 01 0 . 0 C J 0 6 - 2 4 02 .5 6 5 5 4 E 00 3 .4 1 9 3 2 E —01 1. 16128E--0 2 5 . 3 5 4 2 5 E - 0 4 0 . 0 0 . 0 C J 0 6 - 2413 .9 2 6 5 3 E 00 3 . 9 4 1 1 I E — 02 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 4 27 .6 3 6 3 8 E 00 8 . 6 3 1 9 8 E —02 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 4 38 .8 3 4 0 5 E 00 6 . 5 7 5 64E—02 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 4 41.0 4709E 01 C J 0 6 - 2 4 5
35 1280000 0 0 0 NIC KEL C J 0 6 - 2 4 65 .8 7 0 5 0 E 01 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 4 70 . 0 0 . 0 0 . 0 0 . 0 0 . 0 1 .50000E 0 1 C J0 6 — 2481.5 0000 E 01 0 . 0 0 . 0 4 . 8 0 0 0 0 E 00 0 . 0 0 . 0 C JO 6— 2490 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 5 00 . 0 0 . 0 0*0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 5 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 C J 0 6 - 2 5 20 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 5 30 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 5 40 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 — 2550 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 C J 0 6 - 2 5 67 . 4 1 1 5 2 E - 0 2 0 . 0 2.2 9 9 8 3 E 00 0 . 0 3 . 2 1 0 4 9 E - 0 1 C J 0 6 - 2 5 79 . 0 2 3 5 8 E - 0 3 0 . 0 4 . 3 7 3 0 I E 00 0 . 0 1 .6 8 2 9 3 E — 01 C J 0 6 - 2 5 81 .7 1 4 4 8 E —02 0 . 0 1.71661 E 01 0 . 0 1 . 1 0 7 7 9 E -0 1 C J 0 6 - 2 5 91 . 9 6 4 6 6 E —02 0 . 0 1 .5 7946E 01 0 . 0 1 . 1 7 7 14 E -0 1 C J 0 6 - . : 6 03 . 6 3 6 9 8 E - 0 2 0 . 0 1.63349 E 01 0 . 0 3 . 6 3 9 2 2 E - 0 2 C J 0 6 - 2 6 12 . 7 3 5 7 5 E 00 2 . 4 0 9 9 7 E —01 5 .3 8 3 2 9 E--03 5 . 3 9 5 9 6 E -0 4 4 . 56 925E—06 o . o C J 0 6 - 2 6 2
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C J 1 6 - 2 6 3 C J 16-264 C J 1 6 -2 A 5 CJ 16-266 C J 1 6 - 2 6 7 C J 16-268 C J 1 6 -2 6 9 C J 16-270 C J 16— 271 C J 16-272 C J 1 6 - L 7 3 C J 16-274 C J 16— 275 C J 16“ 276 C J 1 6 -2 7 7 C J 16-278 C J 1 6 -2 7 9 C J 16-280 C J 1 6 -2 8 1 C J 16-282 C J 1 6 -2 8 3 C J 16 -284 C J 1 6 - 2 8 5 C J 16-286 C J 1 6 -2 8 7 C J 16-288 C J 1 6 -2 8 9 C J 16-290 C J 1 6 -2 9 1 C J 16 -292 C J 1 6 - 2 9 3 C J 16-294 CJ 16— 29 5 C J 16-296 C J 1 6 - 2 9 7 C J 16-298 C J 1 6 — 299 C J 16-300 C J 1 6 -3 0 1 C J 16-302 C J 1 6 - 3 0 3 CJ 16-304 C J 1 6 - 3 0 5 C J 16-306 C J 1 6 - 3 0 7 C J 16-308 C J 1 6 -3 0 9 C J 16-310 C J1 6 -3 1 1 CJ 16-312 C J 16-313 C J 16-314 C J 1 6 - 3 1 5 CJ 16-316 C J 1 6 -3 1 7 CJ 16-3 18 C J 16 -319 CJ 16-320 C J 1 6 -3 2 1 C J 16 -3 22 C J 1 6 - 3 2 3 C J 16 -3 24 C J 1 6 -3 2 5 CJ 16-3 26 C J 1 6 -3 2 7 C J 16-328
60
0 . 0 3 4 . 00 . 3 6 . 0
2 . 0 1 5 . 03 . 0 1 . 0 Q » 1 5 . 0
10.131 224000 CR- NAT ROD
5 1 . 55
4 . 3 9 7 - 0 3 2 . 2 6 - 0 5 2 . 3 14 2 . 05 . 4 8 - 0 3 3 . 8 1 93 . 6 2 5 - 0 2 6.01
2 . 6 6 0 . 60 5 0 . 0 1 4 8 6 4 . 7 96. 322
133 226000 5 F E - N A T ROD5 5 . 3 6
9 . 0 2 - 0 3 5 . 98 - 0 5 2 . 3 9 2 . 0 2 8 00.7 . 0 5 - 0 3 2 . 9 0 1100.3 . 0 3 - 0 2 8 . 0 7
2 . 7 2 0 . 53 2 6 . 8 3 - 0 3 3. 188.1 2
135 228000 N I - N A T ROD5 8 . 2 1
0 . 1 0 2 9 1. 83 - 0 6 2 . 5 40. 01 0 5 5 4 . 60 . 0 5 3 3 16.8
2 . 8 0 . 4 9 0 . 0 2 217. 0
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CONTINUATION - 2 21 3
0 . 6 1 7 14 . 92 +06
3 . 5 +06
OF CROSS SECTIONS <3-GROUPt BLANKET) 2 0 0
0 . 3 7 3 0 . 0 101. 225 +06 0 . 0 8652 +06
0 . 3 +06 100.
C J 16-32*5 C J 16-330 C J 1 6 - 33 1 C J 16-33? C J 1 6 - 3 3 3 C J 16-334 C J 1 6 - 3 3 5 C J 16-336 C J 16- 337 CJ 16-338
0 . 2 C J 1 6 - 3 3 9C J 16-340 C J 1 6 - 3 4 1 C J 16-342 C J 1 6 - 3 4 3 C J 16-344 C J l 6 - 3 4 5 C J 16-346 C J 1 6 - 3 4 7 C J 16-348 C J 1 6 - 3 4 9 CJ 16-350 C J 1 6 - 35 1 C J 16-352 C J ) 6 - 3 5 3 CJ 16-354
0 . 0 2 8 8 2 C J 1 6 - 3 5 5CJ 16-356 C J 1 6 - 3 5 7 CJ 16-358 C J 1 6 - 3 5 9 C J 16-360 C J 1 6 - 36 1 C J 16-362 C J 1 6 - 3 6 3 CJ 16-364 C J 1 6 - 3 6 5 C J 16-366 C J 1 6 - 3 6 7 C J 16-368 C J 1 6 - 3 6 9 CJ 16-370
0 . 0 8 9 4 C J 1 6 - 3 7 1C J 16-372 C J 1 6 - 3 7 3 C J 16-3 74 C J 1 6 - 3 7 5 CJ 16-376 C J 1 6 - 3 7 7 C J 16-378 C J 1 6 - 3 7 9 C J 16-380 C J 16-381 C J 16-382 C J 16- 383 CJ 16-3 84 C J 1 6 - 3 8 5 C J 16-386
0 . 0 9 1 C J 1 6 - 3 8 7CJ 16-388 C J 1 6 - 3 8 9
- D V - 1 - 7 1 C J 16-390 C J 16—391 C J 16-392 C J 1 6 - 3 9 3 C J 16-394
61
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4 . 6 8 5 1 , 8 3 8 0 . 0 5 8 1 0 . 4 0 . 20 31 3 . 9 3
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0. 0 5 1 513. 91
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C J 1 6 - 3 9 5 CJ 16-396 C J 1 6 - 3 9 7 C J 16-398 C J 1 6 - 3 9 9 C J 16-400 CJl6—401 CJ 16-402 C J 16- 403 C J 16-404 C J 1 6 - 4 0 5 CJ 16-406 C J 16- 407 CJ 16-408 C J 1 6 - 4 0 9 C J 16-410 C J 1 6 - 4 1 1 C J 16-412 CJl6-413 CJ 16-414 C J 16- 415 C J 16-416 C J 1 6 - 4 1 7 C J 16-418 C J 1 6 - 4 1 9 C J 16-420 C J 16-421 CJ 16-422 C J 1 6 - 4 2 3 CJ 16-424 C J 1 6 - 4 2 5 CJ 16-426 C J 1 6 - 4 2 7 CJ 16-428 C J 1 6 - 4 2 9 C J 16-430 C J 1 6 - 4 3 1 CJ 16-432 C J l 6 - 4 3 3 C J 16-434 C J 1 6 - 4 3 5 C J 16-436 C J 1 6 - 4 3 7 C J 16-438 C J 1 6 - 4 3 9 C J 16-440 C J 1 6 - 4 4 1 CJ 16-442 C J 1 6 - 4 4 3 C J 16-444 C J 16- 445 CJ 16-446 C J 1 6 - 4 4 7 C J 16-448 C J 1 6 - 4 4 9 C J 16-450 C J 1 6 - 4 5 1 C J 16-452 C J 1 6 - 4 5 3 CJ 16-454 C J 1 6 - 4 5 5 CJ 16-456 C J 1 6 - 4 5 7 C J 16-458 C J 16- 459 C J 16—460
62
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15 294240 24 0.
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C J 1 6 - 4 6 1 C J 16-462 C J 1 6 - 4 6 3 CJ 16- 464 C J 1 6 - 4 6 5 CJ 16-466 C J 1 6 - 4 6 7 C J 16-468 CJ 1 6 - 4 6 9 CJ 16-470 C J 1 6 - 4 7 1 C J 16-472 C J 1 6 - 4 7 3 C J 16-474 C J 1 6 - 4 7 5 CJ 16-476 C J 1 6 - 4 7 7 C J 16-478 C J 1 6 - 4 7 9 C J 16-480 C J 1 6 - 48 1 CJ 16-482 C J 1 6 - 4 8 3 CJ 16-484 C J 1 6 - 4 8 5 CJ 16-486 C J 1 6 - 4 8 7 CJ 16-488 C J 1 6 - 4 8 9 C J 16- 490 C J 1 6 - 4 9 1 C J 16-492 C J 1 6 - 4 9 3 CJ 16-494 C J 16- 495 CJ 16-496 C J 16- 497 C J 16-498 C J 1 6 - 4 9 9 CJ 16-500 C J 16—501 C J 16-502 C J 1 6 - 5 0 3 CJ 16-504 C J 1 6 - 5 0 5 CJ 16-506 C J 1 6 - 5 0 7 CJ 16-508 C J 1 6 - 5 0 9 CJ 16-5 10 C J 1 6- 5 11 CJ 16-5 12 C J 1 6 - 5 1 3 CJ 16-5 14 C J 16 - 5 1 5 CJ 16-5 16 C J 1 6 - 5 1 7 CJ 16—5 18 C J 1 6 - 5 1 9 CJ 16-5 20 C J 1 6 - 5 2 1 CJ 16-5 22 C J 1 6 - 5 2 3 C J 16- 524 C J 1 6 - 5 2 5 C J I A - 5 26
63
3 . 5 8 525 211023 NA-23B
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31 224000 5 1 . 5 5
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CR-NATB
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4 . 4 35*803 . 22
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32 225055 5 4 . 47
3 . 0 5 - 0 5 2 . 2 94 . 0 4 5 . 2 8
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33 226000 55 . 4
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2. 6 5 0 . 5 8 1 0 . 0 06078 . 5 3
35 228000 N I - N A T B
2 .0 2500.1 0 0 0 .
3 . 2 8 0.11
C J 1 6 - 5 2 7 CJ 16-5 28 C J 1 6 - 5 2 9 CJ 16-530 C J 1 6 - 5 3 1 C J 16-532 C J 16— 533 C J 16-534 C J 1 6 - 5 3 5 C J 16-536 C J 1 6 - 5 3 7 C J 16-538 C J 1 6 - 5 3 9 C J 16- 540 C J 1 6 - 5 4 1 C J 16- 542 C J 1 6 - 5 4 3 C J 16-544 C J 1 6 - 5 4 5 C J 16-546 C J 1 6 - 5 4 7 C J 16-548 C J 1 6 - 5 4 9 C J 16-550 C J 1 6 - 5 5 1 C J 16-552 C J 1 6 - 5 5 3 C J 16- 554 C J 1 6 - 5 5 5 CJ 16-556 C J 1 6 - 5 5 7 CJ 16-558 C J 1 6 - 5 5 9 C J 16- 560 C J 1 6 - 5 6 1 CJ 16-562 C J 1 6 - 5 6 3 CJ 16-564 C J 1 6 - 5 6 5 C J 16- 566 C J 1 6 - 5 6 7 CJ 16-568 C J 1 6 - 5 6 9 C J 16- 570 C J 1 6 - 5 7 1 C J 16- 572 C J 1 6 - 5 7 3 C J 16- 574 C J 1 6 - 5 7 5 C J 16-576 C J 1 6 - 5 7 7 C J 16- 578 C J 16—579 C J 16-580 C J 1 6 - 5 8 1 C J 16- 582 C J 1 6 - 5 8 3 C J 16—584 C J 1 6 - 5 8 5 C J 16-586 C J 1 6 - 5 8 7 C J 16-588 C J 1 6 - 5 8 9 C J 16-590 C J 1 6 - 5 9 1 C J 16-59?
6k
58 . 2
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2 . 8 4 0 , 5 1 0. 02321 5 . 2
58 1 XE- 135B135. 2 . 0 9 3
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63 261147 147.
4 . 0 - 0 43 . 0 - 0 32 . 7 - 0 1
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4 . 7 6 1 . 5 7 0 . 0 4 5 . 8 4 0 . 0 50610. 76
64 261148 1 PM-148MB1 4 8 . 1 . 97 6 - 0 7
3 . 0 3 . 09 . 1 9 . 1
30 1. 301.65 261148 1 P M- I486
148. 1 .488 - 0 6
C J 1 6 —593 CO 16- 594 C,116-595 CJ 16-596 C J 16 - 59 7 C J 16-598 C J 1 6 - 5 9 9 CJ 16-600 C J 1 6 - 6 0 1 C J 16-602 C J 1 6 - 6 0 3 C J 16-604 C J 1 6 - 6 0 5 C J 16-606 C J 1 6 - 6 0 7 C J 16-608 C J 1 6 - 6 0 9 C J 16-6 10 CJl6-611 C J 16-612 C J 16- 613 C J 16-6 14 C J 1 6 - 6 1 5 C J 16-616 C J 1 6 - 6 1 7 CJ 16-6 18 C J l 6 - 619 C J 16-620 C J 1 6 - 6 2 1 C J 16-6 22 C J l 6 - 6 2 3 C J 16-624 C J 16-625 C J 16-6 26 C J 1 6- 6 27 C J 16-628 C J 1 6 - 62 9 CJ 16-630 CJ 1.6-631 CJ 16-632 C J 1 6 - 6 3 3 C J 16- 634 C J 1 6 - 6 3 5 CJ 16-636 C J 1 6 - 6 3 7 C J 16-638 C J 1 6 - 6 3 9 CJ 16-640 C J 16-641 C J 16-642 C J 1 6 - 6 4 3 CJ 16-644 C J 1 6 - 6 4 5 C J 16-646 C J 1 6 - 6 4 7 C J 16-648 C J 1 6 - 6 4 9 CJ 16-650 C J 1 6 - 6 5 1 CJ 16-652 C J 1 6 - 6 5 - CJ 16-654 C J 1 6 - 6 5 5 C J 16-656 C J 1 6 - 6 5 7 f j 1.6-65 Pi
65
0 . 0 7 7 70 . 2 3 6544.
67 26?149 1 4 7 . 6
0 . 0 7 7 7 0 . 2 3 6 544 .
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0 . 0 5 5 6 1 . 2 8 - 0 2 4 . 0 3 2 . 0^•527 8 . 5 14 . 3 0 19.
5 « H 1 . 5 5 0 . 0 1 3 3 7 #4 0 . 29 41 4 . 6
76 1 NSFPB0.0
0 . 0 4 0 . 0 40 . 0 7 0 . 070 . 5 0 . 577 1 SSFPB
0.0
0 . 30 . 55 . 0
81181.
0 . 30 . 55 . 0
TA- 181
0 . 0 30 . 3
2 . 03 . 0 1.0
4 . 0 6 . 0 15 . 0 0.1 o o
C J 16- 659 CJ 16-660 C J 1 6 - 6 6 1 CJ 16-662 C J 1 6 - 6 S 3 C J 16-664 C J 1 6 - 6 6 5 C J 16-666 C J 1 6 - 6 6 7 CJ 16-668 C J 16-669 CJ 16-670 C J 16 - 6 7 1 C J 16-672 C J 1 6 - 6 7 3 C J 16- 674 C J 1 6 - 6 7 5 CJ 16-676 C J 1 6 - 6 7 7 C J 16-678 C J 1 6 - 6 7 9 CJ 16-680 C J 1 6 - 6 8 1 CJ 16-682 C J 16- 683 C J 16-684 C J 1 6 - 6 8 5 C J 16-686 C J 16- 687 CJ 16-688 C J 1 6 - 6 0 9 CJ 16-690 C J 1 6 - 6 9 1 C J 16-692 CJ 26 - 693 CJ 16-694 C J 1 6 - 6 9 5 CJ 16-696 C J 1 6 - 6 9 7 C J 16-698 C J 16-699 C J 16-700 C J 1 6 - 7 0 1 CJ 16- 702 C J 1 6 - 7 0 3 C J 16- 704 C J 1 6 - 7 0 5 CJ 16-706 C J 1 6 - 7 0 ? CJ 16-708 C J 1 6 - 7 0 9 CJ 16-7 10 C J 1 6 - 7 1 1 CJ 16-7 12 C J 1 6 - 7 1 3 CJ 16—7 14 C J 1 6 - 7 1 5 C J 16-7 16 C J V ~ ' ' l 7 C » . > ■ 18 Co x .5-/19 CJ 16-7 20 C J 16-721 CJ 16-7 ?.?C J 1^ - 7 23 r.,1 JA - 7 74
66
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5 4
C J 1 6 - 7 2 5 CJ 16-7 26 C J 1 6 - 7 2 7 CJ 16-728 C J 16-729
1RCJ 16-730 CJl6—731 CJ 16-732
3 2 2 2 1 1 1 C J 16 - 7 3 35 0 00. 2500. 0 . 5 C.J 16-73475. 75. 75 . 75. 75 . 7 5 . C J 1 6 - 7 3 5
CJ 16-736003 C J 1 6 - 7 3 7
0 1 7 1 0 0 1 CJ 16-738. 0001 C J 16-739
0 2500. 0 . 9 7 0 .5 CJ 16-740004 C J 1 6 - 74 1
2 9 1 . 22 1 3 2 37 . 7847 2 28. 994 2 13, 4934 2 12. 5066 2 3 0 . C J 16-7420 C J 16—743
2 30. 1 18. 1 18. 2 22. 2 22. CJ 16-744005 C J 1 6 - 7 4 5
228
22 22 22 10 12 16
2220
2221
CJ 16-746 C J 16-747
7 9 11 15 19 21 CJ 16-7482 4 6 14 18 21 C J 1 6 - 74 91 3 5 13 17 21 CJ 16-750
012 CJ 16- 7511 2 4 1 1 CORE A 1 CJ 16-7523 4 4 1 2 CORE A2 C J 1 6 - 7 5 35 6 4 1 3 CORE A3 CJ 16-7547 8 4 2 4 BLNK Cl C J 16-75 59 10 4 2 5 BLNK C2 CJ 16-756
11 12 4 2 6 BLNK C3 C J 16-75 713 16 4 2 7 BLNK B1 C J 16-75817 20 4 2 8 BLNK B2 C J 16—75921 21 1 2 9 RFLTR E CJ 16-76022 22 1 2 10 RFLTR D C J 1 6- 7 61
0 CJ 16-762018 C J 16—763
10 14 16 12 15 11 17 31 32 33 35 25 58 63 64 65 67 7 6 C J 16-76477 CJ 16-765
020 CJ 16-7661 2 C J 1 6 - 7 6 7
10 2 . 2 8 7 - 5 12 7 . 5 0 4 3 - 3 14 8 . 6 7 7 1 - 4 15 3 . 3 5 3 6 - 4 16 6 . 4 2 1 5 - 5 17 2 . 5 5 9 1 - 5 C J 16-76823 . 0 1 7 6 4 25 . 0090585 33.0097856 31.0026187 35. 00137 83 81 1 . 0 —IOC J.16-769
0 CJ 16-7703 4 C J 1 6 - 77 1
10 2 . 3 9 1 5 - 5 12 7 . 8 4 7 5 - 3 14 9 . 9 0 6 1 - 4 15 3 . 8 2 6 8 - 4 16 7 . 3 2 7 1 - 5 17 2 . 9 2 0 1 - 5 C J 16-77223 . 01 8693 25 . 0084032 33. 0100866 31.0026993 35. 0014206 81 1 . 0 - 1 0 C J 1 6 - 7 7 3
0 C J 16-7745 6 C J 1 6 - 7 7 5
10 2 . 3 5 7 3 - 5 12 7 . 7 3 5 5 - 3 14 1 . 1 5 8 7 - 3 15 4 . 4 7 8 8 - 4 16 8 . 5 7 4 8 - 5 17 3 . 4 1 6 8 - 5 C J 16-77623 *018553 25 . 0082275 33.0101726 31.0027223 35. 0014328 81 1 . 0 - I O C J 16- 777
0 CJ 16-7787 8 C J 16—779
10 2-. 93 95 - 5 12 9 . 3 1 7 6 - 3 25 9 . 0 5 8 5 - 3 33 9 . 7 8 5 6 - 3 31 2 . 6 L 8 7 - 3 35 1. 37 8 3 - 3 C J 16-78023 . 018692 C J l 6—781
9 10 CJ 16-78210 3 . 0 0 P 2 - ^ 12 9 . 8 7 4 7 - 3 25 8 . 4 0 3 2 - 3 3 3 1 0 . 0 8 6 6 - 3 31 2 . 6 99 3 - 3 35 1 . 4 2 0 6 - 3 C J 1 6 - 7 8 323 •01°81 C.i 16—7 8**11 1 2 C J 16-7 8 510 3 . 0 5 4 ; ’ - ^ 1 ?1 0 . 0 2 2 2 - 3 25 8 . 2 2 7 5 - 3 3 3 1 0 . 1 7 2 6 - 3 31 2 . 7 2 2 3 - 3 35 l.*t3 28 —3CJ 16 —7 86?3 . 020105 C J 16—787I ? 20 CJ 16-7 8810 4 . 3 1 8 3 - * 1? 1 *» . 1 7 - 3 2* 4 . 2 2 4 ^ - 3 33 9 . 9 3 3 3 - 3 31 2.658 2 - 3 35 1 . 3 9 9 1 - 3 0 J 1 6 - 78 923 .028426 CJ 16-790
67
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102 8
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33 . 030715 31 8 . 2 1 9 6 - 3 35 4 . 3 2 6 1 - 3
1.0-01 1
2 5 - . 0 0 1 3 0 1 8 1 3 3 . 0 0 1 8 378 131.0004931613 3.0002 5957
- 0 1 11.0
1 2 - . 0 0 0 9 9 7 14.00067 15.00026 16. 00005 17.00002
10 11 12 14 15 16 1758 .0715 . 0 6 .06
. 07 15 . 0 663 . 02 7 . 0 3 .03
.027 . 0367 . 01 3 . 02 .02
. 01 3 . 0276 1. 5011 1.54 66 1.5466
1. 5 011 1. 546677 . 0134 . 0 1 3 4 . 0 1 34
. 01 34 . 0134
.0715
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1.5011
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0361 2 7
5 12 142 10 114 5639000 64 674 5631000 65 2671 581 761 77
0091
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3 10
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7 . 8 6 9 7 - 0 3
7 . 5 8 6 8 - 0 3
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CJ16 C J 16 CJ16 C J 16 CJ16 CJ 16 CJ16 C J 16 C J 16 C J 16 CJ16 C J 16 C J 16 CJ 16 CJ16 C J 16 CJ16 C J 16 CJ16 CJ16 CJ16 CJ 16 C J 1 6 ‘ CJ16' CJ16- C J 16' CJ16- CJ16- CJ16- C J 16' CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ16- CJ 16- CJ16-
14CJ16- CJ16- CJ16- CJ16- CJ 16- CJ16- CJ 16- CJ16- C j 16- CJ16- C J 16*
, CJ16- C J 16- C J 1 6 - C J 16 C J 1 6 - CJ 16- C 1 £>— CJ 16- C J i f'.~ L.i )*-
- 79 1 -792 - 7 9 3 -794 - 7 9 5 -796
797758
- 7 9 9 - 800 -801 -802 - 8 0 3 - 8 04 - 8 0 5 - 8 06 - 8 0 7 -808 - 80 9 -810 -811 -812 -813 -814 -815 - 8 16 - 817 -818 -819 -8 20 -821 -8 22 - 822 - 824 -825 -8 26 -827 -828 -829 -830 -831 -832 -833 -834 -835 -836 -837 -838 -839 -840 -841 -842 -843 -344 -845 -846 -847 -84884985085185?8538 5 4
855
68
1 1 ? . 286060 0 0 1. 0 1. 0 1. 0 1. 02 L 3 .328170 0 0 1 . 0 1. 0 1. 0 1. 03 1 4 .3 84 870 0 0 1 . 0 1. 0 1. 0 1. 04 1
1 . 0 1 . 0 1 . 0 1. 0 1 . 0 1 . 0 1 . 05 1
1 . 0 1 . 0 1 . 0 1. 0 1 . 0 1. 0 1 . 06 1
1 . 0 1 . 0 1 . 0 1. 0 1 . 0 1. 0 1. 07 1
1 . 0 1 .0 1 . 0 1. 0 1 . 0 1. 0 1. 01 200
1 . 0 1 .0 1 . 0 1. 0 1 . 0 1. 0 1. 0093- 0 1 1
0 . 0 11. 0
1 1 1 1 0 0 0 1 0 0 1 1 1 02 1 2 2 0 0 0 1 0 0 1 1 2 03 1 3 3 0 0 0 1 0 0 1 1 3 04 1 4 4 0 0 0 1 0 0 1 1 4 05 1 5 5 0 0 0 1 0 0 1 1 5 06 1 6 6 0 0 0 1 0 0 1 1 6 07 1 7 7 0 0 0 1 0 0 1 1 0 16
00999
o.
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0.0.
0. 0025
0 . 99 6
0 . 996
0 . 99 6
0 . 9 9 6
0 . 9 9 6
0 . 99 6
0 . 9 96
0 . 9 9 5
0 15 19 0 14 18 0 13
C J 16-85 7 CJ 16-858 C J 16-859 C J 16—H60 CJ 16- 8 61 CJ 16-862 C J 1 6 - 8 6 3 CJ 16-864 C J 1 6 - 8 6 5 C J 16-866 C J l 6 - 8 6 7 C J 16- B 68 C J 1 6 - 8 6 9 CJ 16-870 C J l 6 -871 CJ 1 6 - H 7 2 C J 16- R7 3 C J 16-874 C J l 6 - 8 7 5 C J 16-876 C J 16-877 CJ 16-878 C J 1 6 - 8 7 9 CJ 16-880 C J 1 6 - 8 8 1 CJ 16-882 C J 1 6 - 8 8 3
17CJ 1 6- 88 4 C J 1 6 - 8 8 5 CJ 16-886 C J 16- 887 CJ 16-888
TABLE 3
» » » » » » » * » » C I T f t T I t ) N - R E V IS IO N 2 ( J U L Y 1S71I - SUPPLEMENT 2 IMARCH
» » » » » » » ♦ < . TH IS JOB MAS RUN UN 0 3 -1 1 - 7 2 ON THE IBM 360/91*********
ONE-DTMENSIQNAL SLAB ( X I . __________________________________________________ ._________34X7 GROUPS, 238 P O IN T S . STREAM OF C I T A T I O N CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 I 1 1 1 1 0 0
0 0 0 0 0 0
C I O 0 0 0
00
C O O 0 0 0
0 1 0 0 0 0
00
00
00
00
200 100 10 2 3 0 0 l.OOOOOOE 02 9 .9 9 9 9 9 9 F -0 5
0 0 0 9 .99S999E 09
0 0 0 9.9999S9E
023
0 0 0 0 . 0
0 5 6 l.OOOOOOE
1200
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 0 1 0 0 0 0 0 1 1 0 1 0 0 0 0 0 1 0 0 0 09 .9 9 9 9 9 9 E -0 5 1 .0 0 P 0 O 0 E -0 5 0 . 0 0 . 0
9 .9 9 9 9 9 9 E —05 l.OOOOOOE 00
9.99 9 9 9 9 E- 1 .OOOOOOE
-0500
9 . 9 9 9 9 9 J E -0 5 5 . OOOOOOE—01
0 . 00 . 0
L E F T ,T O P ,R IG H T ,B O T T O M ,F R O N T ,B A C K BOUNDARY CO K O IT IC h S AREOTO 070 4 . 6 S 2000E-0 i 070 4 .6 9 2 0 0 0 E -0 1 4 .6 V 2 0 U 0 E -0 1
~ 0 H r in MEM510WAL SLAB G M M FTH V m — ffTTTm— /.OOUOTEF'in--------------------------------------------------------------
REGION S P E C IF IC A T IO N S PTS REGION WIDTH
§ l.OOOOOOE 01 3 l.OOOdCOE Ol 5 l.OOMOOb 01 5 2.0a0000E 01 5 2 . OOOOOOE 01
X - D I R . POfNTS 54
DISTANCES TO MESH INTFRVAL INTERFACES
J2
B i r r r1 .2 5 0 3 2 .5 0 0 4 3 .7 5 0 5 5 .0 C 0 6 6 .2 5 0 7 7 .5 0 0 8 8 .7 5 0 9 1 0 . 0 0 0 10 1 1 .2 5 0
11 1 2 .5 0 0 12 1 3 .7 5 0 13 1 5.000 14 1 6 .2 5 0 15 1 7.500 16 I d . 750 17 2 0 . 0 0 0 18 2 1 .2 5 0 19 2 2 .5 0 020 2 3 .7 5 0 21 2 5 .0 0 0 22 2 6.250 23 2 7 .5 0 0 24 2 8 .7 5 0 25 3 0 .0 0 0 2b 34 .0 0 0 27 3 8 .0 0 0 28 4 2 .0 0 029 4 6 .0 0 0 30 5 0 .0 0 0 31 5 4 .0 0 0 32 5 8 .0 0 0 33 6 2 .0 0 0 34 6 6 . 0 0 0 35 7 0 .0 0 0
'0ISTOCP5 TCI' FLUX POINTS
J1
D I S T .0 .6 2 5 2 1 .8 7 5 3 3 .1 2 5 4 4 .3 7 5 5 5 .6 2 5 6 6 .8 7 5 7 8 .1 2 5 8 9 .3 7 5 9 1 0 .6 2 5
10 1 1 .8 7 5 11 1 3 .1 2 5 12 14 .3 7 5 13 1 5 .6 2 5 14 16.&7S 15 1 8 .1 2 5 16 19.375 17 2 0 .6 2 5 18 21 .8 7 519 2 3 .1 2 5 20 2 4 .3 7 5 21 25 .6 2 5 22 2 6 .B 7 5 23 2 8 .1 2 5 24 2 9 .3 7 5 25 3 2 .0 0 0 26 3 6 .0 0 0 27 4 0 .0 0 023 4^>.OO0 29 4B.0 0 i) 30 b z .o d o 31 ^ 6 . UUU i 2 6 0 . 0 0 0 33 6 4 .0 0 0 34 4 8 .6 0 0
ZONF INPUT BY REGION 1 1 1 - 2 2
ZONE NUMBER AT EACH HESH INTERVAL
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34
1 1 I 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 2 2 2 2 2
* .. .
F IS S IO N SOURCE D IS T R IB U T IO N AMD SUM 0 .9 6 7 5 0 0 .0 3 2 5 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 1 .0 0 0 0 0
D ESCRIPTIO N OF REACTOR ZONES
ZN TO ZN SUB-ZNS SIG M A -S ET 10 CLASS OPL NEX NAME1 1 0 0 0 2 2 0 0 0
1 0 0 2 0 0
COREREFLECTOR
PERTURBATION INPUT - SECTION 0400 0 0 0 0 0 0 0 0 0 0 0 0 . 0 0 . 0 0 . 0
CORE STORAGE DIFFERENCE (WORDS) EQUATION CONSTANTS 1/0 INSTEAO OF STORED 618
EQUATION CONSTANTS MILL BE STORED IN CORE
NUMBcR OP-------COLUMNS* ROWS* PLANTS, GROUPS r UPSCAT, DOWNSCAT, REGIONS, AND ZONES 34 1 1 7 3 3 5 2
MEMORY LOCATIONS RESERVED FOft DATA STORAGE------- 40000MEMORY LOCATIONS USED FOR T H IS PROBLEM----------------- 4830MEMORY LOCATIONS NOT USED----------------------- --------------------------- 35170
INPUT S P E C IF IE D UPSCATTEft s 3 HAS BEEN CHANGED TQ ACTUAL UPSCATTER = 4
ZONE MACROSCOPIC CROSS SECTIONS
T B N F NAME. 6 ftp b SIGR StGA NUSIGF BSQ POWER/FLUX1 CORE 1 2.38400E 00 1 .1 9 8 0 0 E —02 9 .6 1 4 0 0 E— 05 1 .0 7 4 0 0 E -0 4 0 . 0 1.07403E 02
2 1.22100E 00 3 .5 4 6 0 0 E —03 1 .9 8 1 3 0 E—03 6 .2 0 7 0 0 E -0 4 0 . 0 6 .2 0 7 0 0 E 023 1.22700E 00 2 .1 4 0 0 0 E — 02 1 . 6 5 5 4 0 E-0 3 1 .8 2 3 0 0 E -0 3 0 . 0 1 .623008 034 1.22500E CO 3 .7 5 8 3 8 E - 0 2 2 . 16750E-03 3 .1 0 4 0 0 E -0 3 0 . 0 3 .1 0 4 0 0 E 035 1.14500E 00 3 .1 3 5 5 0 E -0 2 6 . 5 8 0 0 0 E-0 3 1 .0 0 3 0OE-O2 0 . 0 1.003006 046 9 .9 3 0 0 0 E -0 1 7 .4 4 8 3 4 E -0 Z 1 .1 1 3 8 0 E -0 2 1 .7 2 9 0 0 E -0 2 0 . 0 1 .7 2 9 0 0 E 047 9 . 17500E-01 7 . 130 0 5 E-0 2 2 .1 4 2 9 0 E -0 2 3 . 39000E—02 0 . 0 3 .3 9 0 0 0 E 04
2 ?EFLECTOR 1 1.83900E 00 1 .5 6 2 0 0 E -0 2 5 .6 2 1 0 0 E— 08 0 . 0 0 . 0 0 . 02 9 .4 8 0 0 0 E -0 1 6 .3 6 9 0 0 E - 0 3 2 .4 9 7 0 0 E -0 6 0 . 0 0 . 0 0 . 03 9 .3 2 9 0 0 E -0 1 2 . 9 8 6 0 0 E -0 2 2 .0 2 8 0 0 E -0 5 0 . 0 0 . 0 0 . 04 4 .^ 5 2 5 5 5 -5 1 7 .6 8 9 2 7 E —02 6 .0 4 3 0 0 E -0 5 0 . 0 0 . 0 0 . 05 8 .9 3 2 0 0 E -0 1 3 .9 3 S 2 0 E -0 2 1 . 1 7 2 0 0 E -04 0 . 0 0 . 0 0 . 06 7 .9 7 1 0 0 E -0 1 8 .3 8 7 0 6 E —02 1 . 9 1 0 0 0 E -0 4 0 . 0 0 . 0 0 . 07 7 . 7 3000E-01 7 .7 2 4 1 4 E - 0 2 3 .4 1 9 0 0 E -0 4 0 . 0 0 . 0 0 . 0
SCATTERING MATRIX
ZONE GRP TO GRP I 2 3 4 5 6 71 1 0 . 0 1 .1 9 8 0 0 E -0 2 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
2 0 . 0 0 . 0 3 .5 4 6 0 0 E -0 3 0 . 0 0 . 0 0 . 0 0 . 03 0 . 0 0 . 0 0 . 0 2 .1 4 0 0 0 E -0 2 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 7 .8 2 7 0 0 E —04 0 . 0 3 . o 4300Et 02 1 .8 2 1 0 0 E -0 4 1 .8 9 0 0 0 E -0 4
5 0 . 0 0 . 0 0 . 0 1 .0 4 9 0 0 E -0 2 0 . 0 1 .8 5 6 0 0 E -0 2 2 .3 0 5 0 0 E -0 36 0 . 0 0 . 0 0 . 0 1 .2 3 4 C 0 E -0 4 5 .9 4 b 0 0 E -0 2 0 . 0 1*49000E— 027 0 . 0 0 . 0 0 . 0 4 .0 5 1 0 0 E — 05 2 .2 '" 7 0 0 E -0 2 4 . 8 6 9 0 0 E - 02 0 . 0
2 1 0 . 0 1 .5 6 2 0 0 E -0 2 0 . 0 0 . 0 0 . 0 0 . 0 0 . 02 0 . 0 0 . 0 6.36SOOE— 03 0 . 0 0 . 0 0 . 0 0 . 03 0 . 0 0 . 0 0 . 0 2 .9 8 6 0 0 E - 0 2 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 4 . 9 3 £00E-04 0 . 0 7 .6 0 0 0 0 E -0 2 3 .6 1 6 0 0 E— C4 3 .7 5 7 0 0 E—055 Q.O 0 . 0 0 . 0 7 .0 3 1 0 0 E -0 3 0 . 0 2 .8 9 3 0 0 E — 02 3 .4 2 1 0 0 E -0 36 0 . 0 0 . 0 0 . 0 7 .0 6 6 0 0 E - 0 5 6 .4 8 1 0 0 E -0 2 0 . 0 1 .8 9 9 0 0 E -0 27 0 . 0 0 . 0 0 . 0 2 . 1 3700E-05 2 .2 0 9 0 0 E -0 2 5 .5 1 3 0 0 E -0 2 0 . 0
ONE-DIMENSIONAL SLAB I X ) .34X7 CROUPS. 238 PO.INTS'. STREAM OF C IT A T IO N CASES ORNL 72
L IN E RELAXATION W ILL BE DONE ON ROMS - 1 INNER I T E R A T I O N (S )ITE R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 8 .0 4 4 0 2 E 00 1 .0 0 0 0 0 1 6 .0 8 8 0 4 - 1 . 8 9 2 0 9 0 . 0 0 .8 7 2 8 5 4 .2 7 .4 2 6 6 1 E -0 1 1 .0 0 0 0 0 0 .8 3 4 9 8 0 .0 2 2 7 4 0 .0 7 9 2 5 0.0 8 * 9 9 23 2 .2 1 9 2 6 E -0 1 1 .0 0 0 0 0 0 .5 2 0 7 5 0 .2 9 9 9 0 -0 .1 8 7 6 5 0 .8 9 8 2 1 04 - J . .1 1 0 4 4 E - 0 1 1.0 0 0 0 0 - 0 .6 1 1 4 1 - 0 . 2 2 3 9 2 1.73541 0 .9 0 5 5 4 1 ’5 - 5 . 2 0 4 4 0 E - 0 2 1 .0 0 0 0 0 0 . 41664 0 .6 7 7 3 7 0 .8 9 3 5 2 0.9 0 9 3 B56 - 3 . 4 H 1 8 E - 0 2 1 .0 0 0 0 0 0 .6 3 2 S 0 0 .6 9 0 1 7 0 .8 1 7 2 0 0.911)2087 - 2 . 7 0 2 2 2 E - 0 2 I . 00000 0 .7 5 0 7 8 0 .6 9 8 C 0 0 .7 9 5 2 5 0 .9 0 9 2 6 18 - 2 . 1 3 2 4 3 6 - 0 2 I . 00000 0.7 6 7 8 2 0 . 72458 0 .7 8 6 3 1 0 .9 0 7 4 9 79 - 1 . 6 6 2 9 2 E - 0 2 1 .0 0 0 0 0 0 .7 6 3 1 9 0 .7 6 0 2 3 0 .7 8 1 7 7 0 .9 0 5 4 8 6
10 - I . 2 9 0 4 5 E - 0 2 1 .0 0 0 0 0 0.76311 0 .8 1 2 8 2 0 .7 7 9 0 3 0 .9 0 3 5 2 911 - 9 . 9 6 8 2 2 E - 0 3 I . 00000 0 .7 6 2 4 9 0 .8 6 1 1 0 0 .7 7 7 1 6 0 . 9 0 1 7 6 7
" i f " - 7 . 4 T 6 T & E - 0 3 1 .0 0 0 0 0 0 .7 6 2 4 5 0 .8 7 7 0 7 0 .7 7 5 7 8 0 .9 0 0 2 4 913 - 5 . 9 0 1 6 9 E - 0 3 1 .0 0 0 0 0 0 .7 6 2 8 7 0 .8 4 7 7 3 0.7 7 4 7 2 0 .8 9 8 9 7 914 - 4 . 5 3 2 9 9 E—03 1 .0 0 0 0 0 0 .7 6 3 5 5 0 .8 3 0 0 0 0.7 7 3 8 8 0 .8 9 7 9 3 715 - 3 . 4 8 0 2 0 E - 0 3 1 .0 0 0 0 0 0 .7 6 4 2 7 0 .8 1 8 5 5 0 .7 7 3 2 0 0 .8 9 7 0 9 416 -2 . 6 7 1 6 0 E - 0 3 1 .0 0 0 0 0 0 .7 6 4 9 9 0 .8 0 7 7 9 0 .7 7 2 6 4
- 9 . 8 5 8 4 7 E - 0 3 . EXTRAPOLATION WITH 3 .6 8 1 4 0 .8 9 3 9 2 1I f 2 .8 2 2 8 & E -0 4 1 .0 0 0 0 0 - 0 . 1 0 5 3 8 - 0 . 0 6 520 3 .6 1 4 6 9 0 .8 9 3 8 9 918 2 .0 0 2 7 2 E - 0 4 1 .0 0 0 0 0 0 . 70966 0 .6 6 4 1 3 -0 .0 1 4 6 0 0 .8 9 3 8 9 319 1 .4 6 8 6 6 E -0 4 1.0 0 0 0 0 0 .7 3 3 4 8 0 .6 7 0 6 4 0 .7 8 9 8 7 0 .8 9 3 8 9 420 1 .0 9 6 7 3 E -0 4 1 .0 0 0 0 0 0 . 74686 0 .6 9 4 1 8 0 .7 8 6 5 5 0.8 9 3 9 0 02 l 8 . 2 0 l 6 0 E - 0 5 1 .0 0 0 0 0 0 . 74791 0 .7 1 8 3 3 0 .7 8 4 2 0 0 .8 9 3 9 0 8
END OF’EISEHmUgTALCULATION - ITgTTATTTW^TlHE 6.C11 HlMOTgii
CONVERGENCE ifclDlCAflON BV M IN IM IZ IN G THE SUM PF THE SQUARES Of THE RESIOUES - R E L A T IV E ABSORPTION 1 .0 0 00467 K 0 .8 9 3 9 3 5 5
LEAKAGE 1 .1 3 6 9 4 E -0 1 TOTAL LOSSES 5 .5 9 3 4 2 E - 0 1 TOTAL PKOOUCTIONS 5 .0 0 0 0 0 E -0 1 REACTOR POMERtMATTS) l.OOOOOE 06
AOJOtN T Pr o b l e m F o l l o w s ITE R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 3 .1 6 5 6 5 E 00 1 .0 0 0 0 0 6 .3 3 1 3 0 - 0 . 6 8 2 6 1 0 . 0 0 .8 9 3 9 0 62 2 .7 5 7 4 3 E -0 1 1 . 0 0 0 0 0 0 .3 6 2 8 5 0 .1 9 6 1 0 0 . 0 0 .8 9 3 9 0 83 2 .6 2 8 1 5 6 -0 1 1 ;00000 1.21593 0 .4 7 7 0 2 0 . 0 0 .8 9 3 9 0 84 2 .4 4 6 5 2 E -0 1 1 . 0 0 0 00 1 .1 7 5 5 4 0 .8 5 7 4 3 0 . 0 0 .8 9 3 9 0 8$ 2 .1 4 9 9 3 E -0 1 1 .0 0 00 0 1 .0 9 3 7 6 0 .8 4 8 7 0 0 . 0 0 .8 9 3 9 0 86 1 .T 7 2 3 0 E -0 1 1 .0 00 00 1 .0 0 1 5 8 0 .8 1 6 1 7 0 . 0 0 .8 9 3 9 0 87 1 .4 2 1 1 7 6 -0 1 1 . 0 0 0 0 0 0 .9 4 3 9 9 0 .7 9 6 2 5 0 . 0 0 .8 9 3 9 0 88 1 .1 2 6 6 0 E—01 1 . 0 0 0 0 0 0 .9 0 5 3 9 0 .7 9 2 1 5 0 . 0 0 .8 9 3 9 0 69 8 . 899 7 8 E-0 2 1 .0 0 00 0 0 .8 7 8 9 6 0 .7 9 3 1 8 0 . 0 0 .8 9 3 9 0 8
10 7 .0 3 3 2 5 E -0 2 1 . 0 0 0 0 0 0 .8 6 0 6 0 0 .7 9 5 5 8 0 . 0 0 .6 9 3 9 0 8HI S V W T O l - D ? ' ‘ y .a a d o o 0 .B 4 7 6 4 0 .7 4 5 0 4 0 . 0 6 .8 4 3 9 0 812 4 . 4 2 3 3 3 E -0 2 1 . 00 0 0 0 0 .8 3 8 3 8 0 .8 0 0 4 0 0 . 0
1 .9 2 1 7 7 E -0 1 E X TR A P O L A TK • WITH 4 .5 3 6 8 0 .8 9 3 9 0 813 2 . 4 1 0 8 9 E-03 1 . 00 0 0 0 0 .05691 0 .1 0 5 2 5 0 . 0 0 .8 9 3 9 0 81 4 i . i ^ a n t - 0 3 I . 0OOO0 6 .4 9 4 6 6 0 . t O J 4 6 0 . 0 0 .8 9 3 9 0 815 - 5 . 9 3 6 6 2 E - 0 4 1 . 0 0 0 0 0 -0 . 4 9 9 3 9 - 0 . 7 1 2 6 9 0 . 0 0.8 9 3 9 0 81& 4 .3 6 f8:JE—04 i .o o d d O - 6 .7 3 5 3 1 - 0 . 74$7* 0 . 0 0 .8 9 3 9 0 817 - 3 . 5 0 4 1 6 E - 0 4 1 . 0 0 0 0 0 - 0 . 8 0 2 6 2 - 0 . 7 5 7 9 3 0 . 0 0 .8 9 3 9 0 818 - 2 . 9 3 5 5 3 E - 0 4 1 .0 0 00 0 0 .8 3 7 4 3 0 .7 6 4 7 1 0 . 0 0 .6 9 3 9 0 819 — 2 . 6 0 6 5 1 E -0 4 1 .0 0 00 0 0 .8 8 7 6 6 0 .7 7 5 4 8 0 . 0 0.8 9 3 9 0 826 - 2 . 4 5 6 * l E - 0 4 l .O o O d o 0 .4 4 2 1 3 0. '79243 0 . 0 0 . 6 9 3 9 0 6 . . . . .21 - 2 . 2 8 2 2 6 E - 0 4 1 .0 0 00 0 0 .9 2 8 9 2 0 .7 9 2 8 1 0 . 0 0 .8 9 3 9 0 821 - 2 . 6 2 l l ^ E - 0 4 l .o o o O o 6.&8&41 0 .8 1 S 4 4 i >*0 6.49390(4 _ . . ,23 — 1 .7 4 4 6 3 E -0 4 1 .0 00 00 0 .8 6 2 9 9 0 .8 1 1 4 0 0 . 0 0 .8 9 3 9 0 824 - 1 . 4 6 9 2 5E—04 1 . 0 0 00 0 0 .64201 0 .8 2 5 6 5 0 . 0 0 .8 9 3 9 0 825 -1 . 2 1 8 3 2 E - 0 4 1 . 0 0 00 0 0 .8 2 9 0 9 0 .8 3 1 0 4 0 . 0
- 5 . 9 1 6 0 4 E - 0 4 EXTRAPOLATION WITH 4 .8 8 4 6 0 .8 9 3 9 0 826 1 .9 0 7 3 5 E -0 5 1 .0 0 0 0 0 - 0 . 1 5 6 5 4 0 . 0 0 .0 0 .* 9 3 9 0 8
27 1.716616-05 1.00000 0.90002 0.90002 0 .0 0.69390828________ 1 .6 2 1 2 S E -0 5 1 .0 0 0 0 0 0 .9 4 4 4 6 0 .9 4 4 4 6 0 . 0 ______________0.8 9 3 9 0 B
END OF A D JO IN T CALCULATION - ITE R A T IO N TIME O.i015 MINUTES
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF TK.'r RESIDUES - R E LATIV E ABSORPTION 1.0000391 K 0 .8 9 3 9 4 0 6
GROSS NEUTRON BALANCE
GRP L F T LEAKAGE TOP LEAKAGE R I T LEAKAGE BOT LEAKAGE FNT LEAKAGE BAK LEAKAGE B**2 LOSSES 1/V LOSS XENGN LOSSX2
0 . 00 . 0
0 . 00 . 0
4 .9 5 3 5 0 E -0 3 1 . 84458E-02
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
34
0 . 00 . 0
0 . 00 . 0
4 .4 3 2 3 8 E -0 3 6 . 6 2 7 59E-03
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
56
6 . 60 . 0
0 . 00 . 0
5 .1 5 6 0 0 E -0 2 2 .0 7 7 4 5 E —02
0 . 00 . 0
0 . 00 . 0
0 . 0G.O
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
7 0 . 0 . 0 . 0 6 . 9001 0 E-0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
S u n 0 . 0 0 . 0 1 .1 3 6 9 4 E -0 1 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
g r p ABSORPTIONS O UT-SCA TTER SOURCE IN -S C A T T E R TOTAL LOSSES TOTAL GAINS PROU/ABSCRPl2
3 .2 6 3 6 0 E -0 31 .3 0 2 3 6 E -0 1
5 .3 2 9 2 8 E -0 14 .0 2 4 2 4 E -0 1
5 .4 1 1 6 3 E -0 1 1 . 81786E-02
0 . 05 .3 2 9 2 8 E -0 1
5 .4 1 1 4 5 E -0 15.5110toE-01
5 .41163E— 01 5 .5 1 1 0 b E -O l
1 .11698E 00 3 .1 3 1 2 0 E -0 1
34
1.7 2 8 9 2 E— 02 2 .4 5 4 9 7 E -0 2
3 .9 2 3 4 4 E -0 18 .7 2 0 9 1 E -0 1
0 . 00 . 0
4 .1 4 0 6 5 E -0 19 .0 3 2 7 1 E -0 1
4 .1 4 0 6 5 E -0 19 .0 3 2 6 8 E -0 1
4 .14065E— 01 9 .0 3 2 7 1 E -0 1
1.0 9 3 8 8 E 00 1.4.1131E 00
56
1 . ^ 6 ^ 6 8 - 6 1 7 .4 4 0 1 3 E -0 2
£.~2 i 66l~l 66 1 .8 1 3 2 6 E 00
0 . 06 . 0
2 .4 2 4 ? 0 E 00 1 .9 0 8 4 3 E 00
2 .4 E 4 7 1 E 00 1.90B44E 00
2 . 42470E 00 1.9 0 8 4 3 E OU
1 .48109E 00 1 .4B886E 00
7 3 .9 3 6 2 0 E -0 2 5 .3 6 9 1 3 E -0 1 575 5 .8 3 1 7 5 E -0 1 5 .8 3 1 7 5 E -0 1 5 .8 3 1 7 5 E -0 1 1 .50368E 00
■JUS 4 .4 $ 6 4 S E -0 1 6 . ?6657E 00 5 .5 9 3 4 1 E -0 1 6 .7 6 6 57E 00 7 .3 2 5 9 1 E 00 7 .32 5 9 1 E 00
ONE-DIMENSIONAL SLAB <X>.34X7 GROUPS, 23B P O IN T S . STREAM OF C IT A T IO N CASES ORNL 72
PERTURBATION RESULTS------- DELTA— K / (K * D E L T A -S J WHERE S REPRESENTS m a c r o ; CROSS S E C TIO N S . LAMBDAIPHI* M PHI 1 * 3 .3 8 4 9 6 6 E -0 1
COMP1
NAMECORE
GRP1
S IG A ,S IG R »D B * * 2 NU*SIGF -6 .1 0 7 2 2 4 E 01 6 .B 4 3 63 4 E
D I F F . COEF. 01 —4 .9 4 8 5 2 3 E—03
B**2 -1 .4 5 5 9 6 2 E 0?
23
-1 . 2 4 3 4 9 3 E 02 1 .3 2 4 5 9 0 E -2 .7 9 2 7 0 6 E 01 2 .0 8 9 2 4 4 E
02 —5.8 5 2 3 6 0 E- 01 - 1 . 7 4 H 6 9 E -
-03-0 3
— 1 . 518304E 02 — 3c 426648E 01
45
— 3 .114774E 01 2 .2 4 5 0 1 2 E —6 .4 8 1 0 9 3 E 01 4 .6 2 2 1 5 1 E
01 - 2 .581008 E- 01 1 .245184E-
-03- 02
— 3 . 815594E 01 -7 . 4 2 0 8 4 7 E 01
6f
-1 .8 0 6 1 5 5 E 01 1•277359E -5 .0 0 3 6 0 3 E 00 3 .4 8 6 8 8 6 E
01 7 . 100739k- 00 2.743«*37E-
-03-0 3
- 1 . 793512E 01 -4 .5 9 0 8 0 5 E 00
2 REFLECTOR 12
— 1.110557E 01 1•245941E - 3 . 7 4 0 9 9 7E 01 3 .8 6 3 6 0 6 E
01 —2 .293273E* 01 - 6 .1 0 2 2 8 9 E -
-02-02
-2 .0 4 2 3 1 3 E 01 — 3.546465E 01
34
-9 .2 6 5 7 9 9 E 00 8 .1 2 5 8 4 7 E - 9 . 130649B 00 8 .0 1 1 1 8 4 E
00 — 1 .60527.0E— 02 00 —1 .6 7 1 8 8 4 £ — 02
-8 .6 4 4 0 6 3 8 00 -8 .6 1 2 0 2 7 E 00
56
— 5.5 0 3 3 2 0 E 01 4 .8 9 8 5 6 3 E -2 .2 8 6 1 3 3 E C l 2 .0 4 1 4 3 8 E
01 —5 . 145096E—02 01 -1 . 6 5 1 6 4 2 E - 0 2
-4 .9 1 5 5 6 S E 01 -1 .8 2 2 2 7 6 E 01
7 - 7 . 605890E 00 6 .8 0 4 5 1 3 E 00 —4 .5 4 5 8 6 4 E --03 -5 .8 7 9 3 5 3 E 00
COMP1
NAMECORE
GRP.1
K ------- SIGS(FRQM ALL GRPS. KK TO GRP. K )6.107224E 01 1 .1 8 2 0 5 5 E 02 1 .8 6 4 4 1 7 E 01 2*003413E 01 4 .1 2 4 5 9 4 E 01 1.139836E 01 3.11 1 4 4 9 E 00
2 6.424321E 01 1 .243493E 02 1.9 6 1 6 8 7 E 01 2.108206E 01 4 . 3 4 4 582E 01 1.201251E 01 3 .2 8 0 0 9 2 E 00
3 9.155978E 01 1.772067E 02 2 .7 9 2 7 0 6 E 01 2.998022E 01 6 .1 4 5 3 6 4 E 01 1.694637E 01 4 .6 2 0 2 0 6 E 00
- ' 4 9.5 1 3 8 8 1 E 01 1 .8 4 1 2 8 2 E 02 Z.9 0 1 5 6 6 E 01 3 . 1 14774E 01 6 .3 8 2 1 1 5 E 01 1.75 9 5 3 1 E 01 4 .7 9 6 4 9 2 E 00
5 9.6 6 0 5 7 0 E 01 1 .869635E 02 2.9 4 6 2 6 9 E 01 3.162930E 01 6.481Q93E 01 1 .7 8 6 8 2 7E 01 4 .8 7 0 8 8 5 E 00
6 9.763335E 01 1.B89495E 02 2 .9 7 7 6 2 1 E 01 3.196754E 01 6 .5 5 1 0 0 4 E 01 1.806155E 01 4 .9 2 3 6 4 9 E 00
7 9.91 7 8 8 9 E 01 1.919374E 02 3.0 2 4 8 1 2 E 01 3 .2 4 7 6 9 3E 01 6 .6 5 6 6 5 0 E 01 1.835417E 01 5.00 3 6 0 3 E 00
2 REFLFCTOR 1 1.110557E 01 3 .4 4 4 0 2 9 E 01 7 .2 4 3 5 7 4 E 00 7.141937E 00 4 .3 6 7 3 8 3 E 01 1.820097E 01 6 .066779E 00
2 1.208717E 01 3 .7 4 0 9 9 7 E 01 7 ,8 6 2 7 9 9 E 00 7 .7 3 4 6 9 5 E 00 4 .7 1 9 5 5 6 E 01 1.966135E 01 6 .5 5 2 2 8 4 E 00
3 1 .4 4 9 6 6 3F 01 4 .4 2 7 9 4 5 E 01 9 .2 6 5 7 9 9 E 00 9.0 5 3 4 8 1 E 00 5 .46 1 7 9 0 E 01 2 . 2 70123E 01 7.556673E 90
4 1.467511E 01 4 .4 7 3 1 2 0 E 01 9 .3 5 3 7 7 1 E 00 9.1 3 0 6 4 9 E 00 5 .4 9 8 3 9 0 E 01 2 .2 8 4 4 8 2 E 01 7 .6 0 3 0 6 5E 00
5 1 .4 7 1 391E 01 4 .481937E 01 9 .3 7 0 0 8 1 E 00 9 . 1 4 4 105E 00 5 .5 0 3 3 2 0 E 01 2«286256E 01 7.6C8516E 00
6 1.473202E 01 4 .4 8 5 3 87E 01 9 . 375829E 00 9 . 146006E 00 5 .503474E 01 2 .266133E 01 7 . 607795E 00
7 1 .4 7 5 5 9 5 E 01 4 .4 8 9 6 9 9 E 01 9 .3 8 2 749E 00 9 . 1 5 2 4 9 7E 00 5 .5 0 3 0 7 3 E 01 2.28 5 6 9 3 E 01 7.605890E 00
END OF CASE - TOTAL CPU TIME WAS 0 .0 5 M N u t E S 1 0t AL CLOtK T lM E HAS 0 .6 1 MINUTES *********************************************************************************************.->************************* *******************************************************************************************************
*********j H IS JOB HAS RUN ON* 0 3 -1 1 -7 2 CN THE IBM 360/91*********
QNE-0IMENSIONAL CYLINDER I R t .34X7 GROUPS, 238 POINTS. STRPAM OF C IT A T IO N CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 1 0 0 0 0 01 1 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
200 100 10 2 1 . OOOOOOE 02 9
3 0 0 .9 9 9 9 9 9E— 05
0 0 0 9 .9 9 9 9 9 9 E 09
0 0 0 9 .9 9 9 9 9 9 E
023
00 . 0
0 0 01
5 6 12 .OOOOOOE 00
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 0 2 0 0 0 0 0 1 1 0 1 0 0 0 0 0 1 0 0 0 09 .9 9 9 9 9 9 E -0 5 1 .0 0 0 0 0 0 E -0 5 9 .9 9 9 9 9 9 E -0 5 0 . 0 0 . 0 1 . OOOOOOE 00
9.9 9 9 5 9SIE-05 1 . OOOOOOE 00
9 .9 9 9 9 9 9 E -0 5 1 . OOOOOOE 00
0. 0O .C
L E F T .T O P .R IG H T ,B O T T O M ,F R O N T .B A C K BOUNDARY C ONDITIONS ARE______________________________________0 . 0 0 . 0 4 .6 9 2 0 0 0 E -0 1 0 . 0 4 . 6 9 2 0 0 0 E - Q I 4 .6 9 2 0 0 0 E -0 1
ONE DIMFNSIONAL CYLIN DRIC AL GEOrtfcTRY <R) WIDTH 1.071700E 02
r e g i o n Sp e c i f i c a t i o n sRTS REGION WIDTH______________________________________________________________________________________________________________
8 2 .2 3 9 0 0 0 E 01 8 2 .2 3 9 0 0 0 E 01 8 2 .2 3 9 0 0 0 E 01 5 2 . OOOOOOE 01 5 2 . OOOOOOE 01
X - D I R . POINTS 34 1
DISTANCES TO MESH INTERVAL INTERFACES
J D I S T . 2 7 .9 1 6 3 1 1 .1 9 5 4 13.711 5 1 5 .8 3 2 6 17.701 7 1 9 .3 9 0 a 2 0 .9 4 4 9 2 2 .3 9 0 10 2 6 .2 5 5
11 2 9 .6 1 9 20 5 4 .2 7 0
1221
3 2 .6 3 95 7 .0 8 4
1322
35.4025 9 .7 6 5
1423
3 7 .9 6 46 2 .3 3 1
1524
4 0 .3 6 46 4 .7 9 6
1625
4 2 .6 2 96 7 .1 7 0
1726
4 4 .7 8 07 1 .6 1 8
1827
4 8 .1 5 27 5 .8 0 6
1928
5 1 .3 0 27 9 .7 7 4
29 8 3 .5 5 4 30 8 7 .1 7 C 31 91 .5 2 0 32 9 5 .6 7 3 33 9 9 .6 5 3 34 103.480 35 1 0 7 .1 7 0
DISTANCES TO FLUX POINTS
J H I S T . 1 5 .5 9 7 2 9 .6 9 5 3 12.516 4 1 4 .8 1 0 5 1 6 .7 9 2 6 18 .5 6 5 7 2 0 .1 8 2 8 2 1 .6 7 9 9 2 4 .3 9 9
10 2 7 .9 8 7 19 5 2 .8 0 7
1120
3 1 .1 6 65 5 .6 9 4
1221
3 4.04858 .4 4 0
1322
3 6 .7 0 56 1 .0 6 1
1423
3 9 .1 8 26 3 .5 7 5
1524
4 1 .5 1 26 5 .9 9 4
1625
4 3 .7 1 86 9 .4 3 0
1726
4 6 .4 9 673 .7 4 2
1827
49.75277 .8 1 5
28 8 1 .6 8 6 29 8 5 .3 B 1 30 6 9.372 31 9 3 .6 2 0 32 9 7 .6 8 3 33 10 1 .5 8 4 34 105 .3 4 1
CORE STORAGE DIFFERENCE 1 WORDS) EQUATION CONSTANTS I/O INSTEAD OF STORED 618
iQ U A T t O N CffNSTAWTS~Wl L L K'E STORED HtN ~COkE
RDM BEft'7)F---CDHm NS7 RCHfr, P U A N ES,"SP m D R 7 ' '( J P S C A T B O h N SCAT,"RTG TflNS, AND"ZONES ... 34 1 1 7 4 3 5 2
SlEMORY LOCATIONS RESEftvEI5 FOR' DAT* S T O R A G E -- 4000 0 “ ..... ... ' "MEMORY LOCATIONS USED FOR T H I S PROBLEM----------------- 4832MEMORY LOCATIONS NOT USED-------------------------------------------------- 35168
ONE—DIMENSIONAL CYLINDER IK I .34X7 GROUPS# 238 P O IN T S . STREAM OF C I T A T I O N CASES ORNL 72
L IN E RELAXATION WILL BE PONE ON ROWS - 1 INNER IT E R A T lO N t S t ______________ITER A TIO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 9 .98 7 2 3 E 00 1 .0 0 00 0 1 9 .9 7 4 4 4 - 1 . 9 2 2 4 9 a . o 0 .7 9 8 0 2 02 8 .3 6 3 5 6 E -0 1 1 .0 00 00 0 .9 2 0 1 0 0 .0 1 7 2 1 0 .1 2 2 8 0 0 .8 2 8 8 5 73 2 .3 0 9 9 1 E -0 1 1 . 0 0 0 00 0 .5 0 7 1 8 0 .3 0 2 5 8 0 .1 1 4 4 6 0 .8 5 0 3 4 44 -1 . 3 3 0 2 5 E - 0 1 1 . 0 0 0 0 0 -0 .7 0 8 9 1 - 0 . 1 8 1 4 2 - 0 .5 6 5 6 4 0 .8 6 6 0 6 35 - 6 . 7 4 9 2 5 E - 0 2 1 .0 00 00 0 .4 3 9 8 8 0 .6 7 6 3 1 1.47045 0 .8 7 5 4 6 06 - i . 5 ^ 2 0 ^ - 0 2 1. 60600 0 .4 9 3 5 3 0 .6 8 3 5 4 0 .9 9 5 3 4 0.8 8 0 1 1 47 -2 . 2 8 8 5 9 E - 0 2 1 . 0 0 0 0 <r 0 .61781 0 .6 9 6 5 7 0.9 0 8 8 9 0 .8 8 1 8 4 88 - 1 . 9 2 6 4 8 E - 0 2 1 .0 0 00 0 0.82251 0 . 71272 0 .8 7 6 8 8 0 .8 8 1 9 5 39 - 1 . 6 Z 0 0 2 E - 0 2 1 . 0 0 0 0 0 0 .82472 0 .7 2 8 7 9 0 .8 6 0 6 9 0 - 481224
10 - 1 . 4 4 9 2 2 E - 0 2 1 . 0 0 0 0 0 0 .8 8 0 0 8 0 .7 6 8 3 8 0 .8 5 0 71 0.8 8 0 1 2 0U -1 . 2 6 0 8 4 E - 0 2 1 . 0 0 0 0 0 0 .85741 0 .7 9 5 2 2 0 .8 4 3 7 6 0 .8 7 8 8 9 712 - 1 . 0 7 6 4 0 E - 0 2 1. 00000 0 .8 4 2 9 5 0 .8 3 5 9 2 0 .8 3 8 5 7 0 .8 / 7 6 9 413 -9 . 0 6 8 4 9 E - 0 3 1 .0 0 00 0 0.83341 0 . 67?55 0.8 3 4 5 1 0 .8 7 6 5 7 914 - 7 . 5 6 8 2 4 E - 0 3 1 .0 00 00 0 .8 2 7 0 0 0 .9 0 6 1 3 0 .8 3 1 2 6 0.87 5 5 8 215 - 6 . 2733 3 E-0 3 1 .0 0 00 0 0 . 82263 0 .8 8 8 4 9 0 .8 2 8 6 0 0.87 4 7 1 116 - 5 . 17434E-03 1 .0 0 00 0 0 .8 1 9 6 4 0 . 36988 0.8 2 6 4 1 0 .8 7 3 9 6 217 - 4 . 2 5 2 6 7 E-0 3 1 .0 0 00 0 0 .8 1 7 6 2 0 .8 5 7 4 6 0 .8 2 4 5 8 0 .8 7 3 3 2 518 - 3 . 5 5 5 ^ - 0 3 I . 00 60 6 0 .6 1 6 2 1 0 .8 5 0 3 4 0 .8 2 3 0 4 0 .8 7 2 7 8 929 -2 . 8 5 2 0 2 E - 0 3 1 .0 0 6 0 0 0 .8 1 5 3 0 0 .8 4 3 2 7 0 .8 2 1 7 4
- 1 .3 8 9 3 6 E — 02 EXTRAPOLATION WITH 4 .857B 0 .8 7 0 1 4 720 2 .4 6 0 4 B E -0 4 1.0 0 0 0 0 - 0 .0 8 6 0 3 -0 . 0 6 7 4 3 4.8 0 7 2 2 0.87013921 2 .0 5 9 9 4 E -0 4 1 .0 0 0 0 0 0 .8 3 7 4 2 0 .7 2 1 6 4 -0 .0 0 9 5 5 0 .8 7 0 1 4 022 1 .7 0 7 0 8 E -0 4 t . 00000 0.8 2 8 8 7 0 .7 2 6 6 0 0 .8 9 1 9 6 0 .6 7 0 1 4 5
1 .4 1 1 4 4 E -0 4 1 .0 00 00 0.8 2 6 9 6 0 .7 5 5 8 6 0 .8 7 5 9 4 0 .87 0 1 5 224 1 .1 5 3 9 5 E -0 4 1 .00000 0.81768 0 .7 8 1 5 6 0 .8 6 4 5 8 0 .8 7 0 1 6 025 9 .4 4 1 3 8 E -0 5 1 .0 0 0 0 0 0 . 81828 0 .8 0 8 3 6 0 .8 5 6 1 5 0 .87 0 1 6 8
END OF EIGENVALUE CALCULA TION - ITE R A TIO N TIME 0 .0 1 2 MINUTES
CONVERGENCE IN D IC A liOhl aV M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 2 2 9 K 0 .8701788
LEAKAGE 2 .3 9 2 3 6 E -0 1 TOTAL LOSSES 1 .1 4 9 2 0 E 00 T C T A l PRODUCTIONS l.OOOOOE 00 REACTOR POWER(WATTS) l.OOOOOE 06
A D JO IN T PROBLEM FOLLOWS ITE R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 3.17823E 00 1 .0 00 00 6 .3 5 6 4 5 -0 . 6 6 9 8 7 0 . 0 0.8 7 0 1 6 82 2 .7 6 0 6 0 E -0 1 1 .0 0 00 0 0.3 6 2 9 2 0 .1 6 4 1 7 0 . 0 0 .8701 V i3 2 .6 2 3 7 8 E -0 1 1 .00000 1.21281 C.46C92 0 . 0 0 . 8 7 0 le d4 2 .4 5 0 5 7 E -0 1 1 .0 0 00 0 1 .1 7 9 0 4 0 .8 4 3 0 2 0 . 0 0 .8 7 0 1 6 85 2 , 16040E-01 1 .0 0 00 0 1.0 9763 0 .7 9 8 6 0 0 . 0 0.8 7 0 1 6 86 1 .7 8 8 2 3 E -0 1 l.OOOPO 1 .0 0 6 5 6 0 .8 2 3 6 4 0 . 0 0 .8 7 0 1 6 87 1 .4 4 2 9 5 E -0 1 T . 66656' 0 .95121 0 .8 6 8 4 9 0 . 0 0 .87 0 1 6 8B 1 .1 5 4 3 9 E -0 1 1 .0 0 00 0 0 .9 1 5 4 6 0 .9 1 2 8 2 0 . 0 0 .8 7 0 1 6 89 9 .2 3 4 3 3 E -0 2 1 .0 0 00 0 0 .8 9 2 2 7 0 .9 0 3 7 9 0 . 0 0 .8 7 0 1 6 8
10 7 .4 1 6 8 2 E -0 2 1 .0 00 00 0 .8 7 7 3 5 0 .8 9 2 8 7 0 . 0 .0 .8 7 0 1 6 811 5 .9 9 2 3 2 E -0 2 1 .00000 0 .8 6 7 8 6 0 .8 8 2 4 4 0 . 0 0 .8 7 0 1 6 812 4 . 87289E-02 1 .0 0 00 0 0 . 86192 0 .8 7 5 0 2 0 . 0 0.8 7 0 1 6 8
' ' 17 ' 52 "I.flffBW 0 .8 $ 8 3 2 0 .8 6 ^ 6 5 0 . 0 0 .8 7 0 1 6 814 3 .2 8 3 7 9 E -0 2 1 .0 00 00 0.8 5 6 2 2 0 .8 6 6 1 7 0 . 0
U 9 7 2 6 3 E -0 1 EXTRAPOLATION WITH 6 .2 0 4 4 0 .8 7 0 1 6 B15 - 1 . 17677E-03 1 .00000 - 0 . 0 3 701 - C . 04117 0 . 0 0 .8 7 0 1 6 a16 -1 . 0 9 2 2 6 E - 0 3 1 .0 0 00 0 0.9 2 7 0 8 0 .7 2 5 1 8 0 . 0 0 .8 7 0 1 6 817 - 9 . 5 9 3 9 6 E-0 4 1 .00000 0 . 8774 0 0 .7 6 2 3 0 0 . 0 0 .8 7 0 1 6 818 - 6 . 1 5 ^ 1 1 1 - 6 4 1 .0 06 60 0.84921 0 .7 9 2 0 2 0 . 0 0 .8 7 0 1 6 829 - 6 . 8 0 6 8 5 E-0 4 1. 00 00 0 0.8 3 3 9 9 0 .8 3 5 8 5 0 . 0 0.87 0 1 6 820 -5 . 6 2 4 8 9 E - 0 4 1 .00000 0. 62579 0 .8 7 0 9 3 0 . 0 0 .8 7 0 1 6 821 - 4 . 6 2 4 1 3 E - 0 4 1 .0 0 00 0 0.8 2 1 6 2 C . 90981 0 . 0 0 .8 7 0 1 6 822 -3 . 7 9 3 8 4 E - 0 4 1 .0 0 00 0 0. 82006 0 .9 3 6 3 0 0 . 0 0 .8 7 0 1 6 823 - 3 . 1 1 1 3 6 E -0 4 1 .0 0 00 0 0 .8 1 9 8 0 *1.91678 0 . 0 0 .8 7 0 1 6 8
24 -2 . 5 5 3 4 6 E - 0 4 1 .0 0 0 0 0 0 .6 2 0 4 3 0 .9 0 9 2 0 0 . 0 0 .8 7 0 1 6 a25 - 2 . 0 9 7 4 9 F - 0 4 1 .0 0 0 0 0 0 .8 2 1 2 2 0 .9 0 9 1 9 0 . 0 _________________________
- 1 . 3 4 0 5 4 E - 0 3 EXTRAPOLATION WITH 26 6 .7 7 I 0 9 E -0 5 1 .0 0 0 0 0 - 0 . 3 2 2 7 5
6 .4 1 8 5 0 0 . 0 0 . 0 0
.8 7 0 1 6 a
.87016827 5 .4 3 5 9 4 E -0 5 1.30000- 0 .8 0 2 8 728 4 .4 8 2 2 7 E -0 5 1 .0 0 0 0 0 0 .82461
0 .8 0 2 8 7 0 . 0 0 0 .8 2 4 6 1 0 . 0 0
.870168
.870168
END OF ADJOINT CALCULATION - ITE R A T IO N TIM E 0 .0 1 3 MINUTES
CONVERGENCE IN D IC A TIO N BY M IN IM IZIN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 5 7 2 K 0 .8 702132
GROSS NEUTRON BALANCE
GRP L F T LEAKAGE TOP LEAKAGE R I T LEAKAGE BOT LEAKAGE FNT LEAKAGE BAK LEAKAGE B**2 LOSSES 1/V LOSS XENON LOSS12
0 . 00 . 0
0 . 00 . 0
1 .0 4 6 9 0 E -0 2 3 . 86748E-02
O .G OoO 0 . 0 0 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
34
0 . 00 . 0
0 . 00 . 0
9 . 2B713E—03 1 . 39386E—02
0 . 0 0*0 0 . 0 0*0
0 . 00 . 0
0 . 00 . 0
0 . 0O .Q
0 . 00 . 0
56
0 . 00 . 0
0 . 00 . 0
1 .0 8 5 6 8 E -0 1 4 .3 7 6 4 4 E —02
0 . 0 0 . 00 . 0 b .O
0 . 0OiO
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
7 0 . 0 0 . 0 1 .4 5 3 3 8 E -0 2 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
SUM 0 . 0 0 . 0 2 . 3923 6E-0 1 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
GRP ABSORPTIONS OUT-SCATTER SOURCE IN -S C A T TE R TOTAL LOSSES TOTAL GAINS PROD/ABSCRP12
7 .0 1 0 7 8 E -0 32 .6 4 4 4 8 E -0 1
1.09435E 00 8 .0 8 5 7 5 E -0 1
1 .11185E 00 3 . 73491E-02
0 .0 1 .1 1 1 8 3 E 00 1 .0 9 4 3 5 E 00 1 .13170E 00
1 . .1 U 8 5 E 00 1.13 1 7 0 E 00
1 .11701E 00 3 . 13150c— C l
34
3 .7 5 2 5 3 E -0 2 5 . 12093E-02
7 .8 5 2 5 8 E -0 1 . 1 .69248E 00
0 . 00 . 0
8 . 3 2 0 7 IE —01 8 .3 2 0 7 1 E —01 1 .7 5 7 6 3 E 00 1 .7 5 7 6 2 E 00
8.3 2 0 7 1 E— 01 1.75 7 6 3 E 00
1 .0 9 5 2 iE 00 1.41413E 00
56
3 .0 9 5 4 6 E -0 1 ‘1 .44446E— 01
4 . 16911E 00 3.3 8 3 1 8 E 00
0 . 00 . 0
4 .5 8 7 2 C E 00 4 .5 8 7 2 2 E 00 3 .5 7 1 3 8 E 00 3 .5 7 1 3 9 E 00
4 .5 8 7 2 0 E O0 3 ;5 7 1 3 8 E 00
1.48427E 00 1 .49226E 00
t 7 .5 7 $ 2 7 E -0 2 9 .9 8 9 9 7 E -0 1 1 .0 8 9 3 1 E 00 1 . 0 8 9 3 i t 00 1 .0 8 9 3 1 E 00 1 .51193E 00
SUM 9 . 0 9968E-01 U 2 9 3 1 9 E 01 1 .14920E 00 1 .2 9 3 1 9 E 01 1 .4 C 811E 01 1.4G811E 01
ONE-DIMENSIONAL CYLINDER I R K34X7 GROUPS, 230 POINTS. STREAM OF C IT A T IO N CASES ORNL 72
PERTURBATION RESULTS------- D E L T A -K / (K * D E L T A - 'SI WHERE S REPRESENTS MACRO. CROSS S EC TIO N S . LAMBOA(PHI* M P H I ) = 3 .3 3 7 4 2 S E -0 2
COUP \AME GRP S I G A , S I G R , 06**2 NU*SIGF D I F F . COEF. 8**21 CORE 1 - 6 . 4 8 1 6 1 5E 01 T . 464145E 01 — 8 .7 3 8 7 4 9 E —03 _-1 .5452G 4E 02
2 -1 .3 5 9 9 7 2 E 02 1 .4 7 3 7 0 6 E 02 — 1 .547 2 0 3 E—02 -1 .6 6 0 5 2 6 E 023 - 3 .1 0 4 4 9 4 E 01 2 .3 0 9 6 1 3 E 01 — 3 . 896826E—03 -3 .8 0 9 2 1 U E .014 - 3 . 3 0 6 8 3 7E 01 2.3 7 1 7 7 1 E 01 -4 . 2 3 1 1 2 1 E -0 3 -4 .0 5 0 8 7 3 E 015 —6 .4 3 6 6 9 4 E 01 4 .5 7 1 5 6 1 E 01 9 .0 6 7 1 1 4 E -0 3 — 7 . 370010E 016 - 1 .7 5 1 6 4 9 E 01 1 .2 3 3 9 8 7 E 01 5 .9 6 7 2 7 1 E -0 3 -1 .7 3 9 3 8 8 E 017 —4.797166E 00 3 . 330464E 00 2 .3 7 0 3 4 5 E -0 3 -4 .4 0 1 3 9 9 E 00
2 REFLECTOR 1 - 7 .7 5 1 8 6 1 E 00 8 .9 3 5 4 5 3 E 00 -2 . 1 8 6 3 9 6 E - 0 2 -1 .4 2 5 5 6 7 E 012 -2 .6 1 6 6 4 0 E 01 2 .7 6 6 0 4 8 E 01 -5 . 6 1 5 4 5 0 E -0 2 -2 .4 B 0 5 7 4 E 013 -6 .4 9 8 5 6 9 E 00 5 .8 2 5 1 5 3 E 00 -1 . 4 4 3 0 9 3 E -0 2 -6 .0 6 2 5 1 3 E 004 —6.4 3 0 2 6 5 E 00 5• 767530E 00 — 1 .52 3 9 8 7 E—02 -6.0b5026<= on3 -3 .9 0 8 3 8 8 E 01 3 .5 5 5 7 8 8 E 01 -4 .8 2 7 5 7 0 E -0 2 -3 .4909711: 016 -1 .6 2 6 4 4 8 E 01 1 .48 4 3 4 4 E 01 — 1 .5 8 4 9 1 5 E -0 2 — 1.296442E 017 — 5 .415602E 00 4.9 5 1 5 4 9 E 00 -4 . 5 1 3 8 5 2 E - 0 3 -4 .1 8 6 2 5 9 E 00
COMP NAME 1 CORE
GRP.1
K ------- S1GSIFR0M ALL GRPS.6 .4 8 1 8 1 5 E 01 1 .2 7 9 7 5 3 E 02
KK TQ GRP. K> 2 . 0 0 5 644E 01 2 .0 5 9624E 01 3 .9 6 9 6 5 5 E 01 1 .0 7 1 5 6 2E 01 2 .8 9 2 0 7 6 E 00
2 6 . 887585E 01 1 .3 599 72E 02 2 .1 3 I 5 0 2 E 01 2.188782E 01 4 .2 2 0 I8 9 E 01 1 .13938ZE 01 3 .0 7 5 5 4 6 E 00
3 1.003307E 02 1.982332E 02 3 .1 0 4 4 9 4 E 01 3.181679E 01 & .099458E 01 1 .6 4 2 2 2 6E 01 4 .4 2 5 9 7 7 E 00
4 1.0 4280BE 02 2.0 6 0 2 5 4 E 02 3 .2 2 6 4 3 0 E 01 3.306837E 01 6 .336644E 01 1.706459E 01 4 .5 9 8 7 9 2 E 00 _
5 1.058603E 02 2 .091310E 02 3 .2 7 5 1 4 3 E 01 3.357237E 01 6 .4 3 6 6 9 4 E 01 1.732994E 01 4 .6 7 0 4 7 7 E 00
6 1.069606E 02 2.112936E 02 3 .3 0 9 0 9 1 E 01 3.392410E 01 6.5 0 5 4 7 0 E 01 1 . 751649E 01 4 -7 2 0 9 5 IE QO
7 1.086137E 02 2.145434E 02 3 .3 6 0 1 2 1 E 01 3.4<*5306E 01 6.609117E 01 1.779802E 01 H.797166E 00
2 REFLECTOR 1 7.751861E 00 2.399860E 01 5 .0 5 4 1 2 4 E 00 5 .004572E 00 3 .0856786 01 i . 2 fc8 i i a e 01 4 .297001E 00
2 8 . 4 7228 7E 00 2 .6 1 6 6 4 0 E 01 5 .5 0 6 1 9 9 E 00 5 .4 3 8 5 1 7E 00 3 .3 4 4 S f i i£ 01 1 .395775E 01 4 .6 5 5 1 2 6 b 00
3 I . 0175316 01 3 . 1 0 1 6 05 E 01 6 . 4 9 8 569E 00 6.373912E 00 3.677309E 01 1.6143626 01 5 .3 7 8 2 3 7 E 00
4 1.030470E 01 3 .1 3 4 4 2 4 E 01 6 . 562730E 00 6 . 4 3 0 265E 00 3 .9 0 4 6 3 IE 01 1 .6251506 01 5.413204E 00
5 1.033265E 01 3.1 4 0 8 1 7 E 0 1 6 . 574645E 00 6.44007CE 00 3.908388E 01 1 .6 2 6 5 2 9 c 01 5 ,~{: i - ’48 7E 00
6 1 .034504E 01 3 .143175E 01 6 . 578S95E 00 6.442677E 00 3.908493E 01 1.626448E 01 5.41701<tE 00
7 1.036084E 01 3.14S982E 01 6 . 583089E 00 6.445422E 00 3.908112E 01 1 .6 2 6 1 1 IE 01 5.41 5 6 0 2 E 00
END OF CASE - fO TA L CPU TIME WAS 0 .0 5 MINUTES TCTAL CLOCK T I H E WAS 0 .5 8 MINUTES *****************************************************************************************************************************************************************I************************************************************
* * * * * * * * * IS jQ B HAS RUfcl 6kl 0 3 -1 1 -7 2 ON THE ItJH 360/91*********
o n e - d i m e n s i o n a l s p h e r e i s i .34X7 GROUPS, 238 P O IN T S . STREAM OF C IT A T IO N CASES ORNL 72
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 '0 0 '0 3 0 0 C 0 0 I I 0 1 0 0 0 0 0 1 0 0 0 09 .9 9 9 9 9 9 F -0 5 1 .0 0 0 0 0 0 E -0 5 9 . 9 9 9 Q 9 9 E - 0 5 9 . 9 9 9 9 9 9 E - 0 5 9 . 9 9 9 9 9 9 E - 0 5 0 . 0 ______________________________0 . 0 0 . 0 1 . OOOOOOE 00 l.OOOOOOE 00 l.OOOOOOE 00 0 .0
L E F T ,TO P ,R IG H T ,B O TT O M ,F R O N T ,R A C K BOUNDARY C ONDITIONS ARE0 .0 _______________ 0^0_______________ 4 .6 9 2 ( ,0 0E-01 0 .0 ____________ 4 .6 9 2 0 0 0 E -0 1 4 .6 9 2 0 0 0 E -0 1
OVC DfMENSIONAL SPHERICAL GEOMETRY ( R I WIDTH 1 .3 9 9 9 6 6 E 02
REGION S P EC IF IC A TIO N SPTS REGION WIDTH
8 3 .333299E 01 8 3 .333299E 01 8 3 .33 3 2 9 9 E 01 5 2 . OOOOOOE 01 5 2 . OOOOOOE O f
X - D I R . POINTS 34
DISTANCES TO MESH INTERVAL INTERFACES
J____ D I S T .2 1 6 .6 6 6 3
11 4 6 .T C 0 122 0 .9 9 85 1 .2 0 5
413
2 4 .0 3 755.C31
514
2 6 .4 5 65 8 .3 8 9
615
2 8 .4 9 96 1 .4 0 0
716
3 0 .2 8 56 4 .1 4 1
817
31 .8 8 26 6 .6 6 6
918
3 3.3337 2 .7 0 0
1019
4 1 .1 0 377.871
20 8 2 .4 3 4 21 29 1 1 6 .5 2 9 30
8 6 .5 4 1 1 1 9 .9 9 9
2231
90.291 1 2 4 .5?9
2332
9 3 .7 5 3 1 2 8 .7 5 2
2433
9 6 .9 7 61 3 2 .7 1 5
2534
9 9 .9 9 91 3 6 .4 5 4
2635
1 0 4 .6 3 4 1 3 ? .9 9 9
27 108.891 28 1 1 2 .8 3 9
DISTANCES TO FLUX POINTS
J D I S T .1 1 3 .2 2 8 2
10 4 4 .0 7 9 111 9 .0 7 84 9 .0 5 6
312
2 2 . 6 2 05 3.187
413
2 5 .3 0 55 6 .7 6 0
514
2 7 .5 1 65 9 .9 3 2
615
2 5 .4 1 96 2 .8 0 0
716
31 .1 0 465 .4 2 8
0I f
3 2 .6 2 469.U 1 3
918
3 7 .6 1 97 5 .3 7 4
19 8 0 .2 1 7 20 28 1 1 4 .7 1 4 29
8 4 .5 3 7 1 1 8 .2 8 9
2130
8 8 .4 5 5122 .3 0 6
2231
9 2 .0 5 41 2 6 .6 7 6
2332
9 5 .3 9 21 3 0 .7 6 3
2433
9 8 .5 1 1134 .6 1 0
2534
1 0 2 .3 6 5138 .2 4 9
26 1 0 6 ,8 0 5 27 1 1 0 .9 0 0
CORE STORAGE DIFFERENCE (WORDS) EQUATION CONSTANTS I/O INSTEAD OF STORED 618-
EQUATION CONSTANTS WILL BE STORED IN CORE
NUMBER O r -------COLUMNS , ROWS, PLANES, GKliUPS , UPSCAT, DQWNSCAT, REGIONS, ANJ ZUNES 34 1 1 7 4 3 5 2
MEMORY LOCATIONS RESERVED FOR DATA STORAbE------- 40000H'cMORY LOCATIONS USED FO’* T H IS PKOBLEM------------— 4832MEMORY LOCATIONS NOT USED--------------------------------------------------
.5iU ' i m k34*7 CROUPS, ?.!»8 P O t N l S . o ci7*rte« CASis orks.
T r i t f m B f c *LUX r.KANdC » 6TA MU-1 *U- 2 MU-3 Ki ... 1 .04035P 01 1 ,0 0 00 0 2 1 ,2 0 7 0 9 0 . 0 _ _ *>. 747391i 9»343:>0£-01 1 ,0 0 00 0 i . 02233 0 .0 1 5 1 8 0 .1 4 9 2 9 0 .7 8 8 2 5 73 -2 . 3 7 1 7 0 E - 0 1 1 . 0 0 0 0 0 - 0 . 4 9 1 0 4 -9*2955-2. . Q: 2 0Z M — ^ ' 3 14 - 1 . 4 4 3 0 6 E - 0 * 1 -2 S 0 G 5 0 . 2 6 / 5 8 0 .0 9 7 7 9 0 .8 4 0 0 2 6f. - r . 6 i * 0 7 E - o j 1 . 0 0 0 0 0 0 .4 5 2 2 0 0 .6 6 8 2 6 - 1 . 2 3 6 8 9 0 .8 5 3 2 0 36 - 4 . 2 5 9 8 7 E - 0 2 1 .0 0 00 0 0 .5 1 5 9 9 0 . 6 6 6 2 2 1 .4 9 0 1 7 0 .8 6 0 9 3 87 -2 . 3 4 6 7 6 E - 0 S 1 . 0 0 0 0 0 0 .5 2 7 4 3 0 .6 7 3 0 5 1 .0 5 0 2 a 0 .8 6 4 2 5 98 - 1 . 3 1 0 8 0 E - 0 2 1 . 0 0 0 0 0 0 .5 4 5 4 5 0 .6 8 3 9 1 0 .9 5 0 5 2 0 .6 6 5 8 8 79 - 1 . 0 3 1 5 7 E - 0 2 1 .0 0 0 0 0 O'. 76161 0 .7 0 1 5 3 0 .9 0 9 5 6 0 .8 6 6 3 4 8
10 - 8 . 1 2 4 0 5 E - 0 3 1 . 06 0 0 0 0 .7 9 4 9 9 0 .7 2 9 5 1 0 .8 8 7 8 7 0 .8 6 6 1 8 711 -7 . 0 4 0 9 8 E - 0 3 1 .0 0 0 0 0 0 .8 5 9 6 4 0 .7 4 7 3 3 0 .8 7 4 6 6 0 .8 6 5 7 1 4
” 12 — - 6 . 3 5 4 S 1 E - 0 3 i.OOOCO 0 .8 9 6 1 5 0 .7 8 0 3 4 0 .8 6 5 9 0 0 .8 6 5 1 0 913 - 5 . 7 5 9 6 9 E - 0 3 1 .0 0 00 0 0 .9 0 0 6 7 0 .8 1 2 6 3 0 .8 5 9 7 8 0 .8 6 4 4 7 014 - 5 . 2 5 5 8 8 E - 0 3 1 . 0 0 0 0 0 0 .9 0 7 2 4 0 .8 5 3 5 4 0 .8 5 5 3 7 0 .8 6 3 8 5 015 - 4 . 7 2 5 9 9 E -0 3 I.OOOCO 0 .8 9 4 4 6 0 .8 8 8 8 1 0 .8 5 2 1 2 0 .8 6 3 2 7 616 - 4 . 1 8 2 1 6 E - 0 3 1 . 0 0 0 0 0 0 .8 8 0 7 5 0 .9 1 4 9 7 0 .8 4 9 6 8 0 .8 6 2 7 5 917 - 3 . 6 5 8 3 5 E -0 3 1 . 00 0 0 0 0 . 8710V 0 .8 9 7 0 8 0 .8 4 7 8 3 0 .8 6 2 3 0 3„ lft ...
- 3 . I 7 1 5 6 E - 0 3 I . 00660 0 .8 6 3 7 7 0 .8 8 1 2 4 0 .B 4 6 41 0 .8 6 1 9 0 619 - 2 . 7 3 1 9 8 E - 0 3 1 .0 0 00 0 0 .8 5 8 6 7 0 .8 7 1 1 9 0 .8 4 5 3 1 0 .8 6 1 5 6 220 - 2 . 3 4 0 7 3 E - 0 3 1 . 0 0 0 0 0 0 .8 5 4 4 5 0 .8 6 3 7 2 0 .8 4 4 4 6 0 .8 6 1 2 6 721 -1 . 9 9 7 8 3 E - 0 3 1 . 0 0 0 0 0 0.85151 0 . 85898 0 .8 4 3 8 0
- 1 . 1 8 2 6 6 E - 0 2 EXTRAPOLATION WITH 5 .9081 0 .8 5 9 5 2 122 1 .3 0 6 5 3 E -0 4 1 .0 00 00 - 0 . 0 6 5 2 7 - 0 . 0 7 5 0 7 5 .8 2 4 9 8 0 .8 5 9 5 2 92* l . t * 4 8 ? 6 - 0 4 1 .0 0 00 0 0. 86873 0 .7 5 1 7 8 - 0 . 0 1 2 3 5 6 .8 5 9 5 3 824 1 .0 0 1 3 6 E -0 4 1 .00000 0 .8 8 2 4 5 0 .8 0 3 0 2 0 .8 6 7 8 0 0 .8 5 9 5 4 925 8 .9 6 4 5 4 E - 0 5 1 . 0 0 0 0 0 0 .8 9 5 3 3 0 .8 3 5 S 0 0 .8 6 2 4 6 0 .8 5 9 5 5 926 8 .0 1 0 8 6 E - 0 5 1 . 0 0 0 0 0 0 .8 9 3 7 0 0 .8 7 1 8 8 0 .8 5 8 7 9 0 .8 5 9 5 6 827 7 .2 4 7 9 2 E - 0 5 1 .0 0 00 0 0 .9 0 4 8 3 0 .9 1 4 6 7 0 .8 5 6 1 8 0 .6 5 9 5 7 7
ENO OF EIGENVALUE CALCULATION - ITE R A T IO N T IM E 0 .0 1 5 ■HIn CiTES
CONVERGENCE IN D IC A T IO N BV M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A T IV E ABSORPTION 1 .0 0 0 0 2 3 b K 0 .8 5 95346
LEAKAGE 2 .4 7 2 3 4 E -0 1 TOTAL LOSSES 1 .1 6 3 3 6 E CO TOTAL PRODUCTIONS l.OOOOOE 00 REACTOR POmcR(mATTS) l .OOOOOE 06
A D JO IN T PROBLEM FALLOWSIT E R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K •
1 3 . 17881E 00 l.OGOCO 6 .3 5 7 6 2 - 0 . 6 6 9 6 8 0 .0 0 .6 5 9 5 7 72 2 .7 6 2 9 0 E -0 1 1 . 0 0 0 0 0 0.3 6 3 2 1 0 . ! 5*J07 0 . 0 0 .8 5 9 5 7 73 2 .6 3 2 1 8 E -0 1 1 .0 0 00 0 1.2 1591 0 .4 5 6 0 6 0 .0 0 .6 5 9 0 7 74 2 .4 5 4 5 9 E -0 1 1 .0 0 0 0 0 1 .1 7 7 9 9 0 .8 2 7 6 7 0 .0 0 .6 5 9 5 7 7$ ' i . 166816-01 i . 00000 1 .0 9 9 4 4 0 .7 7 8 3 0 0 .0 0 .8 5 9 5 7 76 1 .7 9 5 4 8 E -0 1 1 . 0 0 0 0 0 1 .0 0 8 1 8 0 .7 9 0 6 4 0 . 0 0 .6 5 9 5 7 77 1 .4 5 0 6 6 E -0 1 1 .0 0 0 0 0 0 .9 5 3 0 2 0 .8 2 8 3 3 0 . 0 0 .6 5 9 5 7 78 1 . I 6 2 6 1 E -0 1 1. 00 0 00 0 .9 1 7 7 0 0 .8 7 3 6 7 0 . 0 0 .6 5 9 5 7 79 9 .3 2 3 3 1 E - 0 2 1 .0 0 0 0 0 0 .8 9 5 1 6 0 .9 1 0 6 4 0 . 0 0.fc59577
10 7 . 5 1 3 8 1 E -0 2 1 . 0 0 00 0 0 .8 8 1 0 5 0 .9 3 9 4 2 0 . 0 0 .6 5 9 5 7 711 6 .0 9 7 B 9 E -C 2 i.e o o o o 0 .8 7 2 5 4 0 .9 4 4 6 1 0 . 0 0 .6 5 9 5 7 712 4 .9 8 7 1 4 E - 0 2 1 . 0 0 0 0 0 0 .8 6 7 7 2 0 .9 3 070 0 . 0 0 .8 5 9 5 7 713 4 . 1 1 0 3 4 E -0 2 1 .0 00 00 0 .8 6 5 2 9 0 . 92139 0 . 0 0 .6 5 9 5 7 714 3 .4 1 2 8 2 E - 0 2 1 .0 0 0 0 0 0 .8 6 4 4 3 0 .9 1 3 1 4 0 . 0 0 .6 5 9 5 7 71 5 " 2 . 853 1 1 E-0 2 1 .0 0 0 0 0 0 .8 6 4 5 3 0 .9 0 6 3 1 0 . 0
2 . 1 4361E-01 EXTRAPOLATION WITH 7 .7 2 7 6 0 .£ 5 9 5 7 716 - 4 . 62433fe-03 1 .0 0 0 0 0 - 0 . 1 4 5 0 7 -0 . 0 9 7 3 5 0 . 0 0 .8 5 9 5 7 717 —3 . 31980c— 03 1 .0 0 0 0 0 0.8 2 1 6 1 0 .7 4 6 9 5 0 . 0 0 .8 5 9 5 7 718 - 2 . 7 0 7 7 2 E - 0 3 1 .0 0 0 0 0 0 .8 1 2 9 2 0 .7 5 8 4 7 0 .0 0 .6 5 9 5 7 719 — 2 . 1945 8 E-0 3 1 . 0 0 0 0 0 0 .8 0 8 3 0 0 .7 7 6 6 2 0 .0 0 .8 5 9 5 7 7
Coo
2021
-1 .7 7 3 0 0 E -0 3 1.00000 0.80613 0.7904V 0 .0— 1.43123E—03 1.00000 0.80580 0 79977 0 .0
0•859577 0 .8 5 9 5 7 7
2223
-1 .1 5 6 6 3 E 1 -C3-9 . 3 6 8 0 6 E - 0 4
l.OOCOO I . 00000
0.8 0 6 9 80.80901
0 .8 2 7 6 C0 .8 3 8 7 9
0 . 00 . 0
0 .6 5 9 577 0 .8 5 9 5 7 7
2425
- 7 . 6 1 1 5 1E-0A -6 . 2 0 7 2 3 E - 0 4
1 .0 0 0 0 0 3 .0 0 0 0 0
0 .8 1 1 7 3 0 .8 1 4 8 8
0 .8 6 4 C 3 0 . 8914o
0 . 0C .O
0 .6 5 9 5 7 70 .8 5 9 5 7 7
26?7
-5 . 0 8 3 6 8 E - 0 4- 4 . 1 8 1 2 7 F - 0 4
1.0 0 0 0 01 .0 0 0 0 0
0 .8 1 8 4 9 0 .8 2 2 0 7
0 .9 0 8 6 8 0 .9 3 302
0 . 00 . 0
0 .8 5 9 5 7 70 .6 5 9 5 7 7
2629
- 3 . 4 5 2 9 0 E - 0 4- 2 . 8 6 2 8 1 E - 0 4
1.300001 .0 0 0 0 0
0 .8 2 5 4 60.8 2 8 8 2
0 .9 4 9 7 70 .9 5 4 6 7
0 . 00 . 0
0 .8 5 9 s 7 70 .6 5 9 5 7 7
30 - 2 . 3 8 2 4 0 E - 0 4 - 1 . 887 5 7 E-0 3
1 .0 0 0 0 0 0 .8 3 1 9 5 EXTRAPOLATION WITH
0 .9 4 4 5 6 0 . 0 7 .9 4 8 8 0 .6 5 9 5 7 7
3132
1 . 163 4 8 E-0 4 9 . 1 5 5 2 7 F -0 5
1.0 0 0 0 01.00000
- 0 . ^ 8 8 2 5 - 0 . f8698
-0 .0 2 8 3 60 .0
0 . 00 . 0
0 .6 5 9 5 7 70 .6 5 9 5 7 7
33 7 . 4 3 8 6 6 E-0 5 l.OUOOU 0 .8 1 2 5 7 0 .8 1 2 5 7 0 . 0 0 .8 5 9 5 7 7
END OF A D JO IN T CALCULATION - IT E R A T IO N TIME 0 .0 1 7 MINUTES
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THfc SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E A b c-GRPT10N 1 .00 0 0 4 7 7 K 0 .8 5 9 6 1 5 1
GROSS NFUTRON BALANCE
GRP1
L FT LEAKAGE 0 .0
TOP LEAKAGE 0 .0
» I T LEAKAGE 1 .0 9 2 6 6 E —02
BUT LEAKAGE 0 .0
FNT LEAKAGE 0 .0
6AK LkAKAGE 0 .0
B**2 LOSSES 0 . 0
1/V LJS S 0 . 0
XENON LOSS 0 . 0
23
3 . 00 . 0
0 .00 .0
4 .0 1 9 5 3 E -0 2 9 . 64683E—03
0 .00 .0
0 . 00 .0
0 .00 .0
0 .00 . 0
0 . 00 . 0
0 . 00 .0
45
n .o0 .0
0 . 00 .0
1 .4 4 0 0 5 E -0 21 . U 9 & 5 E - 0 1
0 .00 .0
0 .00 .0
O . J0 .0
0 . 00 . 0
0 . 00 . 0
0 .00 .0
67
0 . 00 .0
0 . 00 .0
4 . 51269L—02 1 .4 9 8 3 3 E -0 2
0 .00 .0
0 .0O.C
0 .00 .0
0 . 00 . 0
0 . 00 . 0
0 . 00 .0
SUM 0 .0 0 .0 2 .4 7 2 3 4 E -0 1 0 .0 0 .0 0 .0 0 . 0 0 . 0 0 .0
GRP1
ABSORPTIONS 7 .1 8 4 1 1 F -0 3
OUT-SCA TTER 1 .1 0 7 4 2 E 00
SOURCt I .1 2 5 5 5 E 00
IN -S C A T T E R 0 .0
TOTAL LOSSES 1 . I 2 5 5 3 E 00
TOTAL GAINS 1.1 2 5 5 5 E 00
PROD/ABSCRP 1 .11 7 0 2 E 00
23
2.9 2 3 7 0 E— 01 3 . G4918E-02
8 . 1 2668E- 7 .8 81C5E-
-01■01
3 .7 8 0 9 3E- 0 2 0 . 0
1 .1 0 7 4 2 E 8 . 36244E-
00■01
1 .1 4 5 2 3 E8 .3 6 2 4 4 E -
00-01
1 .1 4 5 2 3 b 8 .3 o 2 4 4 E -
00-01
3 .1 3 1 5 8 E -0 1 1 .09555E 00
45
5 . 1 B 923E-02 3 . 08376E-01
1.6775SE4.08051E
0000
0 . 00 .0
1 .7 4 3 U 9 E4 .5 0 0 8 3 E
CO00
1 .7 4 3 8 9 E4 .5 0 0 8 4 E
0000
1./4 3 8 9 E4 .5 0 0 8 3 E
0000
1.41496E1.48 5 3 5 E
000t>
67
1 . 410Q7E-01 7 . 4 8 C77E-02
3 .3 0 0 5 9 E 00 9 .7 3 4 5 9 E — 01
0 . 00 . 0
3 .4 8 8 7 2 E 1 .0 6 3 2 5E
0000
3 .4 8 8 7 2 E1.06 3 2 5 E
0000
3 .4 8 8 7 2 E1 .06325E
0000
1.4 9 3 4 9 E1.51314E
0000
SUM 9 .1 6 1 2 9 E —01 1.2 7 4 0 4 E 01 1 .1633 6F- 00 1 .2 7 4 0 4 E 01 1.3* 0 3 7 E 01 1 .39037E 01
ONE-DIMENSIONAL SPHERE ( S » .34X7 GROUPS, 238 P O IN T S . STREAM OF C IT A T IO N CASES ORNL 72
PERTURBAT lO‘{ * e S U L T S ----- D ELTA-K /CK*D ELTA-S> .WHERE S REPRESENTS MACRO. CROSS S E C TIO N S . LAMBUAJPHI* M P H I ) = 1 .2 2 3 7 6 9 E -C 5
COHP1
NAMECORE
GRP1
S I 6 A . S I G R , 08**2 NU*SIGF —6.6 1 9 9 1 0 F 01 7 . 71B333E
D I F F . COEF. 01 -1 .1 1 5 5 1 7 E -0 2
a**2-1 .5 / 8 1 8 6 E C2
23
- I . 4 0 3 3 6 0 E 02 1 .5 3 2 5 9 1 E -3 .2 2 3 3 8 4 E 01 2 .3 9 6 3 8 8 E
02 —2 .1 2 7 6 0 9 E— 02 01 - 5 . 2 0 I9 6 O E -0 3
- I . 7135U2E 02 -3 .9 5 5 0 B 9 E 01
45
—3 . 3 79323E 01 2 ;4 2 1 1 4 3 E —6.418312E 01 4 .5 5 1 5 7 2 E
01 —5.4 1 3 8 5 3 E— 03 01 6 .0 6 0 7 0 1 E -0 3
— 4 . 139668E 01 —7 . 348964E 01
A7
-1 .7 3 0 4 1 1 E 01 1 .2 1 6 9 3 3 E -4 .7 1 6 9 1 5 E 0 0 3 .2 6 3 8 5 3 E
01 4 .9 5 2 7 2 5 E —03 00 2 . 0 4 6 8 4 I E - 0 3
— I # 718297E 01 -4 . 3 2 / 7 6 9 E 00 --
2 REFLECTOR 12
*/6 .4 5 2 8 2 IE 00 7 .5 3 0 4 2 7 E -2 .1 8 1 7 0 8 E 01 2 .3 2 9 0 5 7 E
00 - 2 .067273E— 0201 - 5 ,2 5 7 2 0 0 E -0 2
— I . 186674E 01 -2 .0 6 B 2 5 9 E 01
34
-5 .4 2 9 9 7 8 E 00 4 .9 0 3 6 9 3 E -5 .3 4 3 3 0 6 E 00 4 .8 2 8 3 5 7 E
00 —1 . 341830E—02 00 — I .4 1 5 4 9 6 E —02
-5 .0 6 5 6 2 6 E 00 -5 .0 3 9 B 0 5 E 00
56
-3 .2 4 2 0 3 5 E 01 2 .9 7 1 6 3 8 E —1.349172E 01 t .2 4 0 5 0 9 E
01 —4 .5 0 9 1 4 5 E -0 2 01 - 1 .4 9 1 9 4 9 E —02
—2 .8 9 5 7 8 4 E 01 —1.075425E 01
7 - 4 . 4 9 2 4 1 8E 00 4 .1 3 8 2 8 7 E 00 —4 .3 0 0 9 5 6 E — 03 —3 .4 7 2 6 3 8 E 00
COMP1
NAME CORE .
GRP.I
K -----SIGSCFROM A LL GRPS. KIC TO GRP. K 16.6 1 9 9 1 OE 01 1 .3 1 4478E 02 2 .0 5 5 3 4 1 E 01 2.076=579E 01 3 .9 0 3 7 9 9 E 01 1 .043736E 01 2.80 3 6 1 6 E 00
2 7.066814E 01 1 .40 3 3 6 0 E 02 2 .1 9 4 4 0 5 E 01 2.216862E 01 4 .16B 042E 01 1 . U 4 5 1 9 E 01 2 .993S94E 00
- 1.037995E 02 2 .06 2 7 4 9 E 02 3 .2 2 3 3 8 4 E 02 3 .250244E 01 6 .0 79C 89E 01 1.621448E Cl 4 .3 4 9 5 9 6 E 00
4 1.079234E 02 2.14455* ' 02 3 . 3 5 1 155E 01 3.379323E 01 6 .32 0 2 0 7 E 01 1 .68S654E 01 4 .5 2 1 6 3 2 E 00--
5 1.095628E 02 2 .1 7 6 9 7 0 E C2 3 . 4 0 1 874E 01 3.430962E 01 6 .4 1 8 3 1 2 E 01 1 . 7 U 9 7 5 E 01 4 .5 9 2 4 4 3 E CO
6 I .1 0 7 0 1 8 E 02 2 .1 9 9 4 7 9 E 02 3 .4 3 7 1 1 9 E 01 3.466896E 01 6 .4 8 6 8 7 9 E 01 1 .730411E 01 4 .6 4 2 0 9 6 E 00
7 1.124104E 02 2 .2 3 3 2 5 2 E 02 3 .4 9 0 0 1 VE 01 3 .520837E 01 6 .5 9 0 0 I 3 E 01 1.75B171E 01 4 .7 1 6 S 1 5 E 00
2 REFLECTOR 1 6 .4 5 2 8 2 1 E 00 1 .995947E 01 4 .2 0 2 4 7 5 E 00 4 . 1 38288E 00 2 .5 4 7 1 6 3 E 01 1 .063329E 01 3.5 4 7 2 4 8 E CO
2 7 .0 7 1 134E 00 2 . 1 81708E 01 4 .5 8 9 7 0 3 E 00 4 .5 0 7 9 3 4 E 00 2 .7 6 7 5 5 1 E 01 1 .1 5 4 8 2 5E 01 3 .851612E 00
3 8.512380E 00 2 .5 9 2 2 6 5 E 01 5 . 4 2 9 578E 00 5.295538E 00 3 .2 1 5 5 7 9 E 01 1.338871E 01 4 .4 6 0 5 9 5 E 00
4 8 .6 2 2 187E 00 2 .6 2 0 2 0 0 E 01 5 .4 8 4 6 5 5 E 00 5 .343306E 00 3 .2 3 8 8 4 0 E 01 1.348075E 01 4 .4 9 0 4 5 9 E 00
5 8.645601E 00 2 .6 2 5 5 7 5 E 01 5 .4 9 4 7 0 7 E 00 > .3 5 1 5 2 3 E 00 3 .2 4 2 0 3 5 E 01 1 .349252E 01 4.4 9 4 1 3 2 E 00
6 8.65 5 6 1 1 E 00 2 .6 2 7 4 7 7 E 01 5 .4 9 7 8 8 1 E 00 5.353561E 00 3.242C79E 01 1.34 9 1 7 2 E 01 4 .4 9 3 7 0 1 E 00
7 8.668062E 00 2 .6 2 9 6 5 7 E 01 5 .5 0 1 3 3 1 E 00 5.355559E 00 3 .2 4 1 6 5 5 b 01 1.348B56E 01 4.4 9 2 4 1 8 E 00
END OF CASE - TOTAL CPU TIME WAS 0 .0 5 MINUTES . TOTAL CLOCK TIME WAS 0 .6 0 MINUTES .* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * ****************************************************************************************************************
*********t h i s Job waS fcuN on 03- 11-7 2 on the ibm 3&o/ 91 *********7
2 -D PERTURBATION (OLD EXTERMINATQR CASE!_______________________________________9X24X4 GROUPt 864 POINTS STREAM OF C IT A T IO N CASES ORNL 72
CENFRAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 1 O i l I 1 0
0 0 . 0 0 0 0
0 1 0 0 0 0
01
0 0 0 C O O
1 1 0 0 0 0
0Q
00
0Q
00
100 100 10 2 3 0 0 l.OOOOOOE 01 ^ } .9 9 9 9 9 9 E -0 4
0 0 0 9 . 999999E 09
0 0 0 9 .99 9 9 9 9 E
023
0 0 0 0 . 0
0 12 b l.OOOOOOE
1200
6 12 24
NFOTRON FLUX PROBLEM D ESC RIPTIO N - SECTION 003
1 0 0 0 7 0 0 0 0 0 1 0 0 1 0 0 2 0 0 0 0 0 0 09 .9 9 9 9 9 9 E - 0 5 9.-V99999E-05 9.9 9 9 9 9 9 F 29 -4 .0 1 0 0 0 0 E 00
9 .9 9 9 9 9 9E- 0 5 l.OOOOOOE 00
9 .9 9 9 9 S 9 E— 05 1 .0 0 0 0 COE 00
9 .9 9 9 9 9 9 E -0 5 l.OOOOOOE 00
0 . 00 . 0
- '
L E F T ,T O P ,R IG H T ,B O T T O M ,F R O N T ,B A C K BOUNDARY C O N D ITIC h S ,AREC . r 9 .9 9 9 9 9 9 E 29. 9 .9 9 9 9 9 9 E 29 0 .0 9 .9 9 9 9 9 9 E 29 9.9 9 9 9 9 9 E 29
ROD BND. CONSTANTS FOR ZONE2 . 0 P o n r c F - o i 2 . o o o o c o e - o i
22 .0 C 0 0 0 0 E -C 1 0 . 0 -
TWO DIMENSIONAL CYLIN D RIC AL GEOMETRY ( R , Z ) WIDTH 2 .9 9 9 9 9 8 E 01 HEIGHT 4 .6 9 9 9 9 8 E 01 00OO
REGION S P E C IF IC A T IO N SPTS REGION WIDTH
2 6.OOO0OOE 00 2 4 .0 0 0 0 0 0 6 00 3 I .2000006 01 2 6 . C000006 00
, PTS REGION HEIGHT4 8.000000E 00 7 1.4 0 0 0 0 0 E 01 13 2 .5 0 0 0 0 0 E 01 .
X - D J R . POINTS 9 Y -D I R . POINTS 24
OISTANCES TO MESH INTERVAL INTERFACES
J D I S T . 2 4 .2 4 3 3 6 .0 0 0 4 8 .2 4 6 5 1 0 . COO 6 1 5 .1 0 0 7 1 6 .8 6 8 8 2 2 .0 0 0 9 2 6 .3 0 6 10 3 0 .0 0 0
I D I S T .2 2 .0 0 0
11 2 0 .0 0 03 4 .0 0 0
12 2 2 .0 0 0■' 4
136 .0 0 0
23 .9 2 35
148 .0 0 0
2 5 .8 4 66
151 0 .0 0 02 7 .7 6 9
7l b
1 2 .0 0 02 9 .6 9 2
817
1 4 .0 0 03 1 .6 1 5
918
1 6 .0 0 03 3 .5 3 8
1019
1 8 .0 0 03 5 .4 6 2
20 3 7 .3 8 5 21 3 9 .3 0 6 22 4 1.231 23 4 3 .1 5 4 24 4 5 .0 7 7 25 4 7 .0 0 0
DISTANCES TO FLUX POINTS
J D I S T . 1 3 .0 0 0 2 5 .1 9 6 3 7 .211 4 9 .1 6 5 5 12 .8 0 6 6 1 7 .0 8 8 7 2 0 .4 9 4 8 2 4 .2 4 9 9 2 6 .2 1 3
I D I S T .1 1 .0 0 0
1C 19.0002 3 .0 0 0
11 21 •Of'O3
125 .0 0 0
2 2 .9 6 24
137 .0 C 0
2 4 .6 8 55
149 .0 0 0
2 0 .8 0 86
151 1 .0 0 02 8 .7 3 1
716
1 3 .0 0 03 0 .6 5 4
817
1 5 .0 0 03 2 .5 7 7
918
1 7 .0 0 03 4 .5 0 0
] 19 3 6 .4 2 3 20 1 8 .3 4 6 - 21 4 0 .2 6 9 22 4 2 .1 9 2 23 4 4 .1 1 5 24 4 6 .0 3 b
ZONE INPUT BY REGIOK3 2 3 31 2 1 3X 1 I 3
ZONE NUMBER AT EACH MESH INTERVAL
1 2 3 4 5 6 7 8 9
1 3 3 2 2 3 3 3 3 32 3 3 2 2 3 3 3 3 33 3 3 2 2 3 3 3 3 34 3 3 2 2 3 3 3 3 35 1 1 2 2 1 1 1 3 36 1 1 2 2 1 1 1 3 37 1 1 2 2 1 1 1 3 38 1 1 2 2 1 I 1 3 39 1 1 2 2 I 1 1 3 3
10 1 1 2 2 1 1 1 3 311 1 1 2 2 1 1 1 3 312 1 1 1 1 1 1 1 3 313 1 1 1 I 1 1 I 3 314 1 1 1 1 1 1 1 3 315 1 1 1 1 1 1 1 3 316 1 1 1 1 1 1 1 3 317 1 1 1 1 1 1 1 3 318 1 1 1 1 I 1 1 3 319 1 1 1 1 1 1 1 3 3t o 1 I 1 1 1 1 1 3 321 1 1 1 1 1 1 1 3 322 1 1 1 I 1 1 1 3 323 1 1 1 1 1 1 1 3 324 1 1 1 1 1 1 1 3 3
F IS S IO N SOURCE D IS T R IB U T IO N AND SUM 0 .6 0 0 0 0 O .20C00 0 .1 0 0 0 0 0 .1 0 0 0 0 1 .0 0 0 0 0
PERTURBATION INPUT - SECTION 0400 0 0 0 0 0 0 0 0 0 0 0 0.0_______OjO_______0.0
CORE STORAGE DIFFERENCE IWORDSI EQUATION CONSTANTS I/ O INSTEAD OF STORED 139a
EQUATION CONSTANTS MILL BE STORED IN CORE
NUMBER OF-------COLUMNS» ROMS. PLANESt GROUPS. UPSCAT, DOMNSCAT> REGIONS, AND ZONES__________9 24 1 4 3 3 12 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE------ 40000______________________________________________________________________________________MEMORY LOCATIONS USED FOR T H IS PROBLEM--------------- 77 79MEMORY LOCATIONS NOT USED— :------------------------------------------ 32221_______________________________________________________________________________________
20NE MACROSCOPIC CROSS SECTIONS
ZONE NAME________ GRP_________ D______________SIGR____________ SIGA___________NUSIGF____________ BSQ_________ POWER/FLUX1 CSSS 1 5 .0 0 0 2 8 E -0 1 1 . 1 7500 E-0 2 2 .8 0 0 0 0 E -0 2 4 .0 0 0 0 0 E -0 3 1 .0 0 0 0 0 E -0 3 4 .0 0 0 0 0 E 03
___________________________ 2 S . 00 0 2 BE—01 1 .6 7 0 0 0 E -0 2 3 .6 0 0 0 0 E -0 2 8 .0 0 0 0 0 E -0 3 1 .0 0 0 0 0 E -0 3 8 .0 0 0 0 0 E 033 5 .0 0 0 2 5E- 0 1 2 .2 3 0 0 0 E -0 2 6 .0 0 0 0 0 E -0 2 1 .0 0 0 0 0 E -U 2 I.OOOGOE-Q3 l.OOOQOE 04
___________________________ 4 5 .0 0 0 2 BE—01 0 .0 ______________ 9 .0 0 0 0 0 E -0 2 4 .0 0 0 0 0 E -0 2 1 .0 0 0 0 0 E -0 3 4 . 0 OOOOE 04
2 REFLECTOR 1 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0
2 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 .03 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 04 l.OOOOOE 00 0 .0 l.OOOOOE— 04 0 . 0 l.O O O O O E-O v1 u . o
3 I 9 .9 9 0 0 2 E— 01 1 .0 0 0 0 0 E -0 3 1.2 5 0 0 0 E— 04 0 . 0 1 .0 0 0 0 0 E -0 3 0 .0* 9 .9 9 0 C 2 E —01 2 .1 0 0 0 0 E - 0 3 2 . 30000E— 04 0 . 0 l.OOOOOE— 03 o . c3 9 .9 9 0 0 2 E—01 3 .0 0 0 0 0 E -0 3 3 .0 5 0 0 0 E — 03 0 . 0 l.OOOOOE— 03 0 .04 9 .9 9 0 0 2 E—01 2 .0 0 0 0 0 E -0 3 4 . 0 6 0 0 0 E-0 3 0 . 0 l.OOOOOF—03 o . c
SCATTERING MATRIX
ZONE GRPftTO GRP 1 2 3 4
1 1 0 .0 1 .1 0 0 0 0 E -0 2 5 .0 0 00 0 E-04 2 .5 0 0 0 0 E -0 42 2 .0 0 0 0 0 E -0 4 0 . 0 1 . 6 C 000E -0 2 5 .0 0 000E--043 1 .0 0 0 0 0 E -0 4 2 .0 0 3 0 0 6 -0 4 0 . 0 2 .2 0 0 0 0 E -0 24 0 .0 0 . 0 0 . 0 0 . 0
2 1 0 .0 0 . 0 0 . 0 0 . 02 0 . 0 0 . 0 0 . 0 0 . 03 0 . 0 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 0 . 0 0 .0
3 1 0 . 0 5 .0 0 0 0 0 E -0 4 3 .0 0 0 0 0 6 — 0^ 2 .0 0 0 0 0 E - 0 42 ■••000 0OE-O4 O .C 1 .3 0 0 0 0 E— 03 4 .0 0 0 0 0 E -0 43 3 .0 0 0 0 0 E -0 4 6 .0 0 0 0 0 E - 0 4 0 . 0 2 .1 0 0 0 0 E -0 34 2 .0 0 0 0 0 E -0 4 8C000 0 0 E-0 4 1 .0 0 0 0 0 E -0 3 0 . 0
00VJ1
2 -0 PERTURBATION (OLD EXTERMINATOR CASE!9X24X4 GROUP, 864 PO IN TS STREAM OF C IT A T IO N CASES QRNL 72
L IN E RELAXATION WILL BG OONE QN ROMS - 1 1NNER I T E R A T IO N ! S IITE R A TIO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 -7 . 2 3 4 7 7 E - 0 1 I . 00000 - 1 .4 4 6 9 5 0 .0 0 . 0 0 .0 9 9 0 7 12 4 .4 7 3 7 3 E 00 1.76993 - 1 .7 0 9 9 2 - 1 . 7 0 9 9 2 0 .4 9 2 6 0 0 .1 7 1 1 9 73 3.59105E 00 1 .6 2 5 9 3 4 . 39375 0 .1 0 7 9 0 - 0 .1 3 8 9 1 0 .1 7 0 9 5 14 5.5 9 7 6 4 E 00 1 .54713 7.1 5 6 4 1 0 .2 1 3 7 5 -0 .0 2 2 8 2 0 .1 7 2 5 5 75 I . U 9 4 7 E 01 1 .5 0 7 1 7 13.1 9 4 6 3 0 .2 3 4 8 1 7.9 5 4 8 2 0 ,1 7 5 9 7 46 2.42099E 01 1 .4 8 7 6 9 26.3 7 2 5 1 0 .0 9 5 3 8 0 .3 6 9 2 5 0 .1 7 4 5 5 27 3 . 39375E 00 K 4 7 8 3 6 3 .5 3 3 9 3 0 .3 5 6 2 1 3 .9 4 3 0 8 0 .1 7 6 1 2 58 - 5 , 7 6 9 6 4 E - 0 1 1.47394 -0 .7 4 6 9 7 - C . 19567 0 .8 6 7 8 1 0 .1 7 8 0 5 39 - 4 . 8 6 6 4 8 E-0 1 1..47186 0.3 5 6 8 2 0 .6 2 3 6 3 0.7 1 0 4 1 0 .17 9 3 6 1
10 - 3 . 39457E-01 1.4 7 0 8 8 0.3 5 8 0 6 0 .7 3 0 1 6 0 .8 1 3 3 8 0 .1 8 0 4 0 811 -1 .6 9 8 3 9 E - 0 1 1.4 7 0 4 2 0 .3 3 0 4 9 0 .7 8 7 6 6 0 .8 4 0 1 9 3 .1 8 1 2 7 712 1 .4 7 6 2 0 0 .9 2 5 6 2 0 .8 4 5 5 5 0 .8 5 3 9 1 0 .1 8 2 0 4 013 — 1 .9 8 0 1 6 E -0 1 1 .4 7 0 1 0 0 .8 4 7 6 5 0 .8 3 9 2 3 0 .8 3 9 9 0 0 .1 8 2 6 9 614 -1 . 0 7 0 6 6 E - 0 1 1 .4 7 0 0 5 0 .4 3 3 6 3 0 .8 4 5 9 8 0 .8 3 6 1 9 0 .1 8 3 2 5 015 -8 . 6 6 8 3 2 E - 0 2 1.4 7003 0. 72294 C. 84299 0 .8 4 4 2 4 0 .1& 370816 -7 . 9 0 1 0 4 E - 0 2 1.47002 0 .8 3 2 4 7 0 .8 3 6 6 1 0 .8 4 3 3 9 0 ,1 6 4 1 0 317 — 7 .4 1 8 7 3 E -0 2 1.47001 0 .8 6 4 7 7 0 .8 4 1 6 2 0 .8 4 1 7 6 0 .1 8 4 4 3 1 •I s - 6 . 9 5 4 1 5 ^ - 0 2 1.4*001 0 .8 6 7 8 4 0 .8 3 8 3 3 0.8 4 3 8 1 0 .1 8 4 7 0 719 — 6 . 46205E-Q2 1.47001 0.8 6 4 6 2 0 .8 3 5 5 2 0 .8 4 2 0 8
-3 . 9 1 6 9 0 E —01 EXTRAPOLATION WITH 5*6698 0 .1 8 6 2 4 520 3 .5 4 8 3 4 E -0 2 l.COOOO - 0 . 5 1 3 6 2 - 3 , 4 4644 5.6 2 9 9 1 0 .1 8 6 2 3 421 - 2 . 7 4 3 6 3 E - 0 2 1.47001 - 0 . 8006 5 - 0 . 7 1 7 2 2 -0 . 0 0 7 6 1 0 .1 8 6 2 0 622 - 2 . 6 5 7 1 3 E - 0 2 1.4 7001 0 .9 4 1 9 0 0 .8 3 3 9 0 1 .0 6 7 9 7 0 .1 8 6 1 8 023 - 2 . 8 9768E-02 1.47001 1.0 6 1 5 5 0 .8 5 3 0 2 1.0 8 6 4 8 0 .1 8 6 1 5 624 - 3 . 76419E-02 1.4 7001 1 .26139 1 .4 5 8 2 7 0.9 9 8 5 9 0 . 18613b25 4 . 86794E-02 1.47001 - 1 . 2 4 4 5 4 - 0 . 5 7 3 5 0 1.2 0 4 0 9 0 .1 8 6 1 1 326 2 .9 8 2 3 3 E -0 2 1.4 7001 0 .6 4 2 4 7 1 .4 7 4 6 0 0 .9 7 2 9 8 0 .1 8 6 0 8 927 - 2 .8 8 3 9 5 E - 0 2 1.4 7001 -0 .9 9 5 8 5 - 0 . 8 3 6 8 8 0 .6 6 5 4 6 0 .1 8 6 0 7 328 3 .1 0 7 0 7 E -0 2 1.47001 - 1 . 0 4 6 2 9 - 0 . 4 8 5 6 8 1 .1 5 8 2 4 0 .1 8 6 0 5 029 - i . 323 3 9 E-0 2 1.47001 - 0 . 4 3 9 1 6 - 1 . 1 4 2 1 2 0 . t 3 0 5 6 0 .1 8 6 0 3 530 7 . 355 6 9 E-0 3 1.4 7001 - 0 . 54847 - 0 . 0 7 1 0 4 1.0 5 9 5 5 0 .1 8 6 0 1 931 5 .2 6 4 2 B E -0 3 1.47001 0 .7 2 0 9 4 0 .8 4 5 1 5 0 .8 7 7 1 5 0 .1 8 6 0 0 632 5 .0 0 3 9 3 E -0 3 1.47001 0.9 5 5 5 5 0 .8 4 1 5 0 0 .9 0 1 1 9 0 .1 8 5 9 9 433 4 .7 7 7 9 1 E -0 3 1.47001 0.9 5 9 6 1 0 .8 4 0 9 1 0 .8 9 4 3 8 0 .1 8 5 9 8 334 4 .0 9 6 0 3 F -0 3 1.47001 0 .8 6 1 7 8 0 .8 4 0 0 1 0 .8 8 1 1 7 0 .1 8 5 9 7 435 3 . 7 1 S 6 5 E -0 3 1.4 7001 0. 9I 012 0 .8 3 6 5 1 0 .8 7 6 4 3 0 .1 8 5 9 6 636 3 .3 8 2 6 8 E -0 ? 1.4 7001 0.9 1 4 5 1 0 .8 3 1 8 9 0 .8 7 0 4 3 0 .1 8 5 9 5 937 3 .0 2 0 2 9 E -0 3 '1 . 4 7 0 0 1 0. 89589 0 .8 3 5 4 1 0 .8 6 4 7 6 0 .1 8 5 9 5 3 .38 2 .6 8 0 7 8 E -0 3 1.47001 0 .8 9 0 2 7 0 .8 4 9 1 3 0 .8 5 9 4 3 0 .1 8 5 9 4 839 2 .3 5 6 5 3 E -0 3 1.4 7001 0 .8 8 1 4 0 0 .B 4 2 6 9 0 .8 5 3 8 0 0 .1 8 5 9 4 340 2 .0 5 7 0 8 E -0 3 1.47001 0. 87498 0 .8 3 7 4 7 0 .8 4 8 4 0 0 .1 6 5 9 4 04 i I . ? 8 3 S ? E - 0 ? 1.4V001 0 .8 6 8 7 3 0 .6 3 3 0 6 0 .8 4 3 0 4
1 .0 1 5 9 0 E -0 2 EXTRAPOLATION WITH 5 .7 0 6 6 0 .1 8 5 9 1 942 1 .0 6 8 1 2 E -0 4 I . 00000 0 .0 6 0 0 0 0 .5 4 7 7 0 5 .5 5 6 2 0 0 .1 8 5 9 1 S43 9 . 7 2 7 4 8 E -0 5 1.47001 0.91081 1 .5 7 1 3 5 -0 i 0 1 7 8 7 0 .1 8 5 9 2 044 - t . 5 7 5 7 5 E - 0 5 1.47001 -O ' . '77887“ - 0 . 8 0 1 1 7 1.2 7 3 1 8 0 .1 B 5 9 2 0
:N0 OF EIGENVALUE CALCULATION - ITE R A T IO N TIME 0 .0 6 0 MINUTES
C on vergence i n d i c a t i o n by m i n i m i z i n g th e sum o f t h e S q u a re s o f The r e s id u e s - r e l a t i v e a b s o r p t i o n 1 .0 0 0 0 2 0 0 k 0 . 1 6 5 9 2 2 8
LEAKAGE 5 .7 6 4 5 1 E -0 1 TOTAL LOSSES 5 .S ? 8 6 5 E 00 TOTAL PRODUCTIONS 9 . 9 ^ 9 9 E - 0 1 REACTOR POWER!WATTSI 9 .99999E 05
CE30TNT' PROBLEM FOLLOWS ITE R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 2 .0 9 8 9 8 E 02 1.0 0 0 0 0 4 1 9 .T 9 5 9 6 - 1 . 0 3 8 7 2 0 . 0 0 .1 8 5 9 2 02 3 .6 6 7 2 8 E 00 1.7 6 9 9 3 3 .6 8 4 7 6 0 .2 4 6 5 1 0 . 0 0 .1 8 5 9 2 03 1 .0 5 9 2 4 E 00 1 ,6 2 5 9 3 1 .3 4 8 0 8 0 ,6 7 4 6 8 0 .0 0 .1 8 5 9 2 04 7 . 71167E-01 1.5 4 7 1 3 1.4 9 9 2 0 0 .7 4 1 7 1 0 . 0 0 .1 8 5 9 2 0
8 .9 J 6 0 5 E -P 1 1 .5 0 7 1 7 2 .0 4 7 7 8 0 . 94372 0 . 0 o . i a » 9 z o6 5 .8 3 6 0 0 E -0 1 1.46769 1.23815 0 .6 1 8 1 2 0 . 0 0 .1 8 5 9 2 07 3 .0 7 4 7 8 E — 01 1 .4 7 8 3 6 0 .8 3 4 3 4 0 .2 5 6 3 4 0 . 0 0 .1 8 5 9 2 00 2 .0 0 V 5 6 E -0 1 1 .4 7 3 9 4 0 .8 5 2 5 6 0 .6 2 1 C 1 0 . 0 0 .1 8 5 9 2 09 1 .6 1 9 6 3 E -0 1 1 .4 7 1 8 6 0. 96 97 7 0 .6 4 7 5 1 0 . 0 0 . 1 8 * 9 2 0
10 1 .7 8 0 0 0 E -0 1 1 .4 7 0 8 8 1.27702 0 .6 4 0 8 5 0 . 0 0 .1 8 5 9 2 011 2 .1 6 6 6 4 E -0 1 1.47042 1.43388 0 .7 2 8 4 9 G.O 0 .1 8 5 9 2 012 1 .5 2 6 6 7 E -0 1 1 .4 7 0 2 0 0 .8 5 7 2 9 0 .7 5 7 0 7 0 . 0 0 .1 8 5 9 2 013 9 . 0987 2 E-0 2 1 .4 7 0 1 0 0 .6 8 6 9 7 0 .7 5 3 6 7 0 . 0 0 .1 8 5 9 2 014 2 .8 7 0 3 7 E -0 2 1 .4 7 0 0 5 0 .3 4 4 1 7 1 .7 9 3 2 2 0 . 0 0 .1 8 5 9 2 015 -1 . 5 4 8 1 2 E - 0 2 1.47003 -0 . 5 5 4 8 3 - 0 . 3 9 9 2 8 0 . 0 0 .1 8 5 9 2 016 7 . 51495E— 03 1.4 7002 -0 .4 7 7 9 1 - 0 . 6 1 0 0 0 0 . 0 0 .1 8 5 9 2 017 6 .2 6 0 8 7 E -0 3 1.47001 0.8 3 9 3 8 0 .7 4 9 3 2 0 .0 0 .1 8 5 9 2 018 6 .2 1 7 0 0 E -0 3 1.47001 0 .99921 0 .7 4 6 7 0 0 . 0 0 .1 8 5 9 2 019 5 .8 4 7 9 3 E -0 3 1.47001 0 .9 4 6 4 8 0 .7 9 0 0 8 0 . 0 0 .1 8 5 * 2 020 5 .3 3 4 8 5 E -0 3 1.47001 0 .9 1 7 6 0 0 .7 4 3 6 4 0 . 0 0 .1 8 5 9 2 0 .21 4 . 8 1 701E-03 1.47001 0 .9 0 7 7 5 0 .9 2 4 4 0 0 . 0 0 .1 8 5 9 2 0 ■22 4 .4 8 3 2 2 E - 0 3 1.47001 0 .9 3 5 1 9 1 .0 4 5 5 9 0 . 0 0 .1 8 5 9 2 023 3 .9 6 3 4 7 E -0 3 1 .47001 0 .8 8 8 0 3 1 .1 0 5 9 5 0 . 0 0 .1 8 5 9 2 024 3 .8 5 7 6 1 E -0 3 1.470C1 0 .9 7 7 1 5 0 .9 5 8 7 5 0 . 0 0 .1 8 5 9 2 025 4 .1 5 9 9 3 E - 0 3 1 .47001 1 .08253 0 . 9 0 6 90 0 . 0 0 .1 8 5 9 2 026 5 .2 2 8 0 4 E -0 3 1 .47 001 1.26199 1 .6 4 7 0 6 0 . 0 0 .1 8 5 9 2 027 7 .3 5 5 6 9 E -0 3 1 . V J 2 8 6 1.4 1432 1 .0 9 3 9 5 0 . 0 0 .1 8 5 9 2 028 - 7 . 4 7 7 8 2 E - 0 3 1 .4 0 2 8 6 - 1 . 0 2 4 0 8 -0 .6 7 7 4 1 0 . 0 0 .1 8 5 9 2 029 5 .7 1 4 4 2 E - 0 3 1 .4 0 2 8 6 - 0 . 7 5 8 4 7 - 0 . 7 3 2 1 9 0 . 0 0 .1 8 5 9 2 030 1 .8 5 3 9 4 E -0 3 1 .4 0 2 8 6 0 .3 2 6 2 9 0 .8 0 2 6 3 0 . 0 0 .1 8 5 9 2 031 1 .2 3 6 9 2 E - 0 ’ 1*34531 0.66842 0 .0 0 4 4 8 0 . 0 0 .1 8 5 9 2 032 7 . 085 8 0 E-0 4 1.34531 0 . 57357 0 .7 3 7 3 7 0 .0 0 .1 8 5 9 2 033 5 .5 2 1 7 7 E -0 4 1.34531 0. 77983 0 .6 7 1 2 3 0 . 0 0 .1 8 5 9 2 034 4 .8 7 3 2 8 E -0 4 1.3 4531 0 .8 8 3 0 4 0 .4 8 9 7 9 0 . 0 0 .1 8 5 9 2 035 4 .4 4 4 1 2 E - 0 4 1.34531 0.9 1 2 3 8 0 .2 0 8 3 3 0 . 0 0 .1 8 5 9 2 036 3 .9 8 6 3 6E— 04 1 .34531 0 .8 9 7 3 9 0 . 0 0 . 0 0 .1 8 5 9 2 037 3 .5 7 6 2 8 E -P 4 1 .34531 0 .8 9 7 4 9 0 .8 9 7 4 9 0 . 0 0 .1 8 5 9 2 038 3 .2 1 3 8 8 E -0 4 1.3 4531 0 .8 9 8 9 9 0 .8 9 8 9 9 0 . 0 0 .1 8 5 9 2 039 2 .8 8 0 1 0 E -0 4 1.34531 0 .8 9 6 4 3 0 .8 9 6 4 3 0 . 0
2 .4 9 2 3 0 E -0 3 EXTRAPOLATION WITH 8 .6 5 5 3 0 .1 8 5 9 2 040 1 . 14441E— 05 1 .0 0 0 0 0 0 .0 3 9 7 5 Ok 03975 0 . 0 0 .1 8 5 9 2 041 1 .5 2 5 8 8 E -0 5 1 .3 4 5 3 1 1 .3 3 3 3 5 1 .2 3 4 6 9 0 . 0 0 .1 8 5 9 2 042 1 .2 3 9 7 8 E -0 5 1 .34531 0.81251 1 .0 6 6 1 1
o•o
0 .1 8 5 9 2 0
END OF A D JO IN T CALCULATION - ITE R A T IO N TIME 0 .0 4 9 MINUTES- -
t oMve*Genes l N b i a n o n BY H t N I H l Z I N G THE Su M OF THE SQUARES OF THE RESIDUES - R E L A T IV E ABSORPTION 1 .0000143 K 0 .1 8 5 9 2 2 6
66655 NEUTft fiM fell MCE
GRP1
L F T LEAKAGE 0 .0
TOP LFAKAGE 1 .1 7 3 5 8 E-02
R1T LEAKAGE 3 . 17588E-01
BOT LEAKAGE 0 .0
FNT LEAKAGE 0 .0
BAK LEAKAGE 0 .0
B**2 LOSSES 4 .4 2 2 5 3 E — 02
1/V LOSS 0 . 0
XENON LOSS 0 . 0
23
0 . 0 , 0 . 0 *■
5 .2 2 5 1 1 F -0 3 2 .0 5 1 7 9 E - 03-
1 .4 2 0 6 7E-0 1 5 . 5 4 6 9 OE—02
0 .00 .0
0 . 00 . 0
0 . 00 . 0
1 .9 7 4 2 9 E — 02 7 .6 5 2 2 4 E - 0 3
0 . 00 . 0
0 . 00 . 0
4 0 .0 2 . 2 9 6 58E-03 4 .0 0 1 8 5 E —02 0 .0 0 . 0 0 . 0 5 . 72069E—03 0 . 0 0 . 0
SUM 0 . 0 2 .1 3 0 9 3 E -0 2 5 . 5 5142E-01 0 .0 0 . 0 0 .0 7 . 73410E— 02 0 . 0 0 . 0
GRP ABSORPTIONS O UT-S C A TTER SOURCE I N -S C A T T E R T O T A L ’ LOSSES TOTAL GAINS PROD/ABSGRP12
2.63764E flO 1.15687E 00
8 .3 0 4 3 1 ^ -0 15 .2 9 5 2 4 E -0 1
i . i n m (TOl i0 7 5 7 3 E 00
9 .B 2 7 3 0 E -0 3 7 .7 7 7 C 3 E —01
3.23T"02E 06 1 .C 5343E 00
3 .2 3 7 0 2 E do 1.8 5 3 4 3 E 00
1 .3 7 4 9 7 E -0 1 2 . 156 5 6 E-0 1
34
7 .4 1 9 8 6 E — 01 7 .9 2 9 6 2 E -0 1
2 .7 3 9 88E-01 2 . 3 6 1 84E-03
5 .3 7 8 6 5 E -0 1 5 .3 7 8 6 5E—01
5 .4 3 2 8 2 E -0 1 3 .0 5 4 9 3 E —01
1 .0 8 1 1 4 E 00 8 .4 3 3 6 0 E —01
1.0B115E 00 8 .4 3 3 5 8 E — 01
1 .6 2 6 5 3 E -0 1 4 . 4 1 749E—01
IsUM 4.72485E 00 1.63630E 00__ 5 . 37865E 00 1.6363CE 00 7.01495E 00 7.01495E 00
GROUP NEUTRON BALANCE FOR EACH ZONE
ZONE NUMBER 1— CORE VOLUME 5 . 64 8 5 8E 04
GftP ABSORPTIONS O U T-S CA TTER 8**2 LOSSES 1/V LOSS XENON LOSS IN -S C A TTE R SOURCE POMERCMATTSl AVERAGE FLUX12
1.9 5 6 7 6 E 00 1.12 2 6 9 E 00
8 .2 1 1 4 1 E -0 1 5 .2 0 8 C 2 E —01
3 .4 9 4 4 1 E - 0 2 1 .5 5 9 3 7E—02
0 .00 . 0
0 . 00 .0
7 .4 4 4 0 1 E -0 37 .7 1 1 4 1 E -0 1
3 .2 2 7 1 9 E1.07573E
0000
2 .7 9 5 3 7 E 05 2 .4 9 4 8 6 E 05
1 .2 3 7 2 0 E —03 5 .5 2 0 9 9 E — 04
34
7 .2 4 1 1 7 E -0 17 .8 8 1 5 2 E -0 1
2 .6 9 1 3 0 E -0 10 . 0
6 .0 3 4 6 1 E -0 3 4 .3 7 8 8 7 E —03
0 .00 .0
0 . 00 .0
5 .3 3 9 1 4 E -0 12 .9 8 5 7 4 E -0 1
5 . 37865E— 01 5 . 37865E—01
1 .2 0 6 8 6 E 05 . 3 . 50290E 05_
2 .1 3 6 5 8 E -0 41 .5 5 0 3 4 E -0 4
SUN 4 . 5 9 1 7 I E 00 1 . 6 U C 7 E 00 6 .0 9 5 1 3 E -0 2 0 . 0 0 . 0 1.61107E 00 5 . 37865E 00 9 .9 9 9 9 9 E 05
ZONE NUMBER 2— REFLECTOR , VOLUME 4 . 42336E 03
SRP ABSORPTIONS OUT— SCATTER ti**2 LOSSES 1/V LOSS XENON LOSS IN -S C A TTE R SOURCE POWER!WATTS) AVERAGE FLUX12
7 .$ 1 1 7 8 6 -0 2 3 .3 2 3 1 2 E — 02
0 .00 . 0
0 . 00 . 0
0 . 00 .0
0 . 00 .0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
34
1 .2 9 3 0 6 E -0 21 .6 2 0 8 6 E -0 5
0 . 0 . 0 . 0 .
0 . 01 .6 2 0 8 6 E -0 4
0 .00 . 0
0 . 00 . 0
0 . 00 .0
0 . 0a . o
0 . 00 . 0
0 . 03.6 6 4 3 I E - 0 5
SUM 1.2 1 2 9 6 E— 01 0 .0 1 . 62086E—04 0 .0 0 . 0 0 .0 0 . 0 0 . 0
ZONE NUMBER 3— VOLUME 7 . 19801E 04
GRP ABSORPTIONS O U T-S C A TTER B**2 LOSSES t / V LOSS XENON LOSS IN -S C A T TE R SOURCE POWER!WATTS) AVERAGE FLUX12
i . t 6 B o e - 6 r9 . 5 5 2 6 5 E -0 4
9 .2 9 0 4 3 E -0 38 .7 2 1 9 8 E -0 3
9 .2 8 1 1 7 E -0 3'♦.14918E-03
0 . 00 .0
0 . 00 . 0
2 .3B 329E— 03 6 .5 6 1 5 0 E -U 3
0 . 00 . 0
0 . 00 . 0
1 .2 9 0 7 0 E —04 5 .7 7 0 1 0 E -0 5
a4
4.94671te-6S4 .7 9 4 5 2 E -0 3
4 . 657761:-03 2 .3 6 1 8 4 E -0 3
1 .6 l7 6 4 f e -0 i 1 .1 7 9 7 4 E -0 3
o .b0 .0
0 .00 . 0
9 .3 6 7 3 7 E -0 36 .9 1 9 8 5 E -0 3
0 . 00 . 0
0 . 00 . 0
2 .2 4 9 5 8 E - 0 5 1 .6 4 0 6 2 E —05
SUN 1 .1 8 4 9 8 E -0 2 2 .5 2 3 2 0 E -0 2 1 .6 2 2 7 7 E -0 2 0 .0 0 . 0 2 .5 2 3 2 0 E -0 2 0 . 0 0 .0
2 -0 PERTURBATION (010 EXTERMINATOR CASE)9X24X4 GROUP, 864 POINTS STREAM OF C I T A T I O N CASES ORNL 72
POINT POWER O IS T R IB U T IC N (W ATTS/CCI
1 2 3 4 5 6 7 8 91 0 . 0 0 . 0 0 . 0 0 . 0 C.O 0 . 0 0 . 0 0 . 0 0 .02 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0.0 -3 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 .05 1.0 4 3 E 00 9 .7 1 9 E -0 1 0 . 0 0 . 0 1 .546E 00 1 .4 1 3 E 00 1 .0 1 1 E 00 0 . 0 0 .06 1 .6 5 3 E 00 1.477E 00 0 . 0 0 . 0 2 .3 8 4 E 00 2 .1 7 0 E 00 1 .4 9 7 E 00 0 . 0 0 .07 2 .4 7 1 F 00 2 .1 3 9 E 00 0 . 0 0 . 0 3.3 6 0 E 00 3 .0 2 5 E 00 2 .0 4 2 E 00 0 . 0 0 .08 3 .6 2 6 E 00 3 .0 4 7 F 00 0 . 0 0 . 0 4 .5 3 9 E 00 4 . 0 2 I E 00 2 .6 6 7 E 00 0 . 0 0 .09 5.314E 00 4 .3 4 6 E 00 0 . 0 0 . 0 6 .0 0 9 E 00 5 .2 0 C E 00 3 .3 9 1 E 00 0 . 0 0 .0
10 7 .8 2 6 E 00 6 .2 9 8 E 00 0 . 0 0 . 0 7 .8 8 6 E 00 6 .6 0 6 E 00 4 .2 2 5 E 00 0 .0 0 .011 1 .1 5 4 E 01 9 .4 7 4 E 00 0 . 0 0 . 0 1.Q34E 01 H . 2 6 6E 00 5 . 1 74E 00 0 . 0 0 .012 1.663E 01 1.529E 01 1 .404E 01 1 .3 5 3 E 01 1 .3 5 8 E 01 1 .0 1 4 E 01 6 .2 0 2 E 00 0 . 0 0 .013 2 .2 0 8 E 01 2 .0 9 8 E 01 1 .9 8 3 E 01 1 .8 8 0 E 01 1.694E 01 1 .2 1 0 E 01 7 .2 7 2 E 00 0 . 0 0 .014 2 .753E 01 2.6 3 9 E 01 2 .5 0 6 E 01 2 .3 5 3 E 01 2 .0 2 8 E 01 1 .4 1 1 E 01 B .3 6 9 E 00 0 . 0 0 . 015 3 .2 7 2 E 01 3 .1 4 3 E 01 2 .9 8 3 E 01 2 .7 8 4 E 01 2 .3 5 0 E 01 1 .6 0 9 E U l 9 .4 5 7 E 00 0 . 0 0 .016 3 . 7S3E 01 3 .604E 01 3 .4 1 7 E 01 3 .1 7 8 E 01 2 .6 5 3 E 01 1 .7 9 9 E 01 1 .0 5 1 E 01 0 . 0 0 . 017 4 .1 9 0 E 01 4.0 2 2 E 01 3 .8 C 8 E 01 3 .5 3 4 6 01 2 .932E 01 1 .9 7 6 E 01 1 .1 5 0 E 01 0 . 0 0 . 018 4 .5 7 9 E 01 4 .3 9 3 E 01 4 .1 5 6 E 01 3 .8 5 1 E 01 3 .184E 01 2 .1 3 7 E 01 1 .2 4 0 E 01 0 . 0 0 .019 4 .9 1 7 E 01 4 .7 1 6 E 01 4 .4 5 9 E 01 4 .1 2 8 E 01 3 .4 0 5 E 01 2 .2 8 0 E 01 1 .3 2 1 E 01 0 . 0 0 .0
7 3 “ S.203E 01 4 .9 8 8 E 01 4 .7 1 5 E o i 4 .3 6 2 E 01 3.593E 01 2 .4 0 2 E 01 1 .3 9 0 E 01 0 . 0 0 .071 S .4 3 4 E 01 5.208E 01 4 .9 2 1 E 01 4 .5 5 2 E 01 3 .7 4 6 E 01 2 .S 0 2 E 01 1 .4 4 6 E 01 0 . 0 0 .02g 5 .6 0 9 E 01 5 .375E 01 5 .0 7 8 E 01 4 .6 9 6 E 01 3 .8 6 2 E 01 2 .5 7 3 E 01 1 .4 8 9 E 01 0 . 023 5 .7 2 6 E 01 5 .487E 01 5 .1 8 3 E 01 4 .7 9 2 E Q1 3 .9 4 0 E 01 2 .6 2 9 E 01 1 .5 1 8 E 01 0 . 024 5 .7 8 5 E 01 5 .5 4 3 E 01 5 .2 S 6 E Oi 4 .8 4 1 E 01 3 .9 7 9 E 01 2 .6 5 5 E 01 1 .5 3 3 E 01 0 . 0
0.00 . 00.0 00
VO
2 -D PERTURDATION (OLD EXTERMINATOR CASE>9X24X4 GROUP, 864 P O IN TS STREAM OF C I T A T I O N CASES OHNL 72
PERTURBATION RESULTS------- 0 6 L TA -K / ,<K*DEL TA - S I WHERE S REPRESENTS MACRO. CROSS S E C T I O N S . LAMBDAIPHI* M P H I ) = 1 .1 4 4 5 5 7 E -0 2
COMP1
NAMEC0R6
GRP1
S I G A , S I G R ,00**2 — 9 . 706219E 00
NU*SIGF 7 .0 0 7 4 2 2 E 01
O I F F . COEFr - 3 .49 9 0 6 2 E— 02
ti**2 -4 .8 5 3 3 8 0 E 00
23
—6 .1 9 2 7 1 OE 00 - 2 .6 1 8 9 2 1 E 00
3 .1 2 8 1 2 3 E 01 1 .2 1 0 1 6 7 E 01
- 5 . 4 2 8 0 3 6 6 - 0 2 -2 . 2 9 B 1 6 7 E - 0 2
-3 .0 9 6 5 2 S E 00 - 1 . 309525E 00
2 REFLECTOR41
- 3 . 6 2 3 3 1 7E 00 0 . 0
8 .7 1 1 5 1 0 E 00 0 . 0
- 3 . 0 6 9 9 8 9 E - 0 20 . 0
- 1 . S I 17596 00 0 .0
23
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 .0
341
— 1 .6 9 3 0 0 7 E— 02 — I . 86644OE—01
9 .1 0 6 1 1 8 E -0 3 1 .3 1 6 1 1 0 E 00
— 2 .5 4 2 7 4 3 E —04 - 1 . 2 5 7 3 1 0 E - 0 2
-1 . 6 9 3 0 0 7 E -G 2-1 .8 6 4 5 7 6 6 -0 1
23
- 1 . 1 8 2 58 2 E-01 — 4 . 910842E— 02
5 .8 8 5 0 4 3 E -0 12 .2 9 2 8 8 4 E -0 1
- 7 . 9 B 9 4 7 7 E -0 3 — 3 .3 4 6 4 3 5 E -0 3
- 1 . 181402E— 01 — 4 . 905941E— 02
4 - 6 . 4 9 0 1 8 9 E - 0 2 1 .6 5 3 1 8 1 E -0 1 —4 .5 3 5 4 7 0 E —03 -6 .4 8 3 7 1 0 E — 02
COMP FJTm? GRP. K ------ - Sl6S«t-RbM A LL GRPS. KK TO GRP. KI1 CORE______________ 1 9 .7 0 6 2 1 9 E 00 4 .3 3 2 9 0 0 E 00 1 .6 7 6 2 4 6 E 00 1 .206492E 00______________________________________________
2 1 .387244E 01 6 .1 9 2 7 1 0 E 00 2 .3 9 5 7 4 7 6 00 1.724424E CO_____________________________ 3 1 .516475E 01 6 .7 6 9 5 6 2 E 0 0 2 .6 1 8 9 2 1 E 00 1.B85292E 00______________________________________________
4 2 .9 1 3 4 8 7 E 01 1 .3 0 0 5 6 3 E 01 5 .0 3 1 5 0 2 6 00 3 .623317E 002 REFLECTOR 1 0 . 0 _______________ 0^0_______________ OUO_______________ 0^0___________________________________________________________
2 0 .0 0 .0 0 .0 0 .0_____________________________ 3 0 . 0 _______________ 0 .0 _______________ OUO_______________ OjO___________________________________________________________
4 0 . 0 0 . 0 0 . 0 1 .6 9 3 0 0 7 E -0 2 3_______________________ 1 1 .8 6 6 4 4 0 E — 01 8 . 3 4 5 9 0 2 6 -0 2 3 .2 S 1 6 5 7 E -0 2 2 .3 4 3 7 9 5 6 -0 2 _______________________________________________
2 2 .6 4 4 6 7 6 E -0 1 1 .1 8 2 5 8 2 E -0 1 4 . 6 0 7 4 7 9 E -0 2 3 .3 2 1 2 2 8 E -0 2_____________________ ________ 3 2 .8 1 8 8 1 0 F —01 1 .2 6 0 4 4 3 6 -0 1 4 .9 1 0 8 4 2 6 -0 2 3 . 5 4 0 « a i E - 0 2 _______________________________________________
: 4 5 .1 6 2 2 7 8 E -0 1 2 .3 0 8 3 0 4 6 -0 1 8 .9 9 3 5 0 0 6 -0 2 6 .4 9 0 1 8 9 6 -0 2
END OF CAS6 - TOTAL CPU T I N E MAS 0 .1 8 MINUTES TOTAL CLOCK TIM E WAS 1 .4 8 MINUTES *************************************************************************************************************** ***************************************************************************************************************
* ********TH IS JOB WAS RUN ON 0 3 -1 1 - 7 2 ON THE IBM 360/91*********
2 - 0 CASE P6RT1JPBFO TO CHECK PERTURBATION RESUl T , R C . l l CHANGED - . 0 5 9X24X4 GROUP, 864 PO IN T* STREAM OF C I T A T I O N CASES ORNL 72
CENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 0 o e 0 0 0 0 0 I 1 0 0 0 0 01 0 1 1 1 1 0 C O O 0 0 0 0 0 0 0 0 0 0 0 0 0 0
100 100 10 ? 3 0 0 l.OOOOOOE 01 9 .9 9 S 9 9 9 E -0 4
0 0 0 9 .9 9 9 9 9 9 E 09
0 0 0 9 .9 9 9 9 9 9 E
023
00.0
0 0 01
5 6 12 .OOOOOOE 00
6 12 24
F IS S IO N SOIIRCF D IS T R IB U T IO N AND SUM 0 .6 3 0 0 0 0 .2 0 C 0 0 0 .1 0 0 0 0 0 .1 0 0 0 0 1.00000CORE STORAGE DIFFERENCE (WORDSi EQUATION CONSTANTS I/O INSTEAD OF STORED 1395
EQUATION CDNSTAKTS H IL L BE STORED IN CORE______________________________________________________________ ________________ _______________________
NUMBFR OF-------COLUMNS, ROWS. PLANES. GROUPS. UP SCA T. PCHNSCAT. REGIONS. AND ZONES__________ 9 24 1 4 3 3 12 3
MFMOKY LOCATIONS RESEPVEO FOR DATA STORAGE-------- 40C00_______________________________________________________________________________________MEMORY LOCATIONS USED FOR T H IS PROBLEM------------------ 7779MEMORY LOCATIONS NOT USED--------------------------------- --------------- 32221________________________________________________________________________________________
ZONE MACROSCOPIC CROSS SECTIONS
CONE NAME GRP D SIGR SIG A NUS IGF as>g POWkK/FLUX1 COfcc' 1 4 .5 0 0 2 8 E -0 1 1 .1 7 5 0 0 E -0 2 2. 8OCOOE-O2 4 .0 0 0 0 0 E -0 3 1 .0 0 0 0 0 E -0 3 4 . 0 0 0 0 0 E 03
2 5 .0 0 02BE-01 1.6 7 0 0 0 c — 02 3. 600006— 02 8 .0 0 0 0 0 6 -0 3 1 .0 0 0 0 0 E -0 3 8 .0 0 0 0 0 E 033 5 .0 0 0 2 5 E -0 1 2.Z 3 0 0 0 fc-0 2 5 .9 9 9 9 9 E — 02 I.O O O O O E-O 2 1 .0 0 0 0 0 E -0 3 l.OOOOOE 044 5 .0 0 0 2 8 E -0 1 0 . 0 8 .S 9 9 9 9 E -0 2 4 Dooooe-oz 1 .0 0 0 C 0 E -0 3 4 .0 0 0 0 0 6 04
2 RtFLFCTOR 1 0 . 0 0 . 0 0 .0
O•o
0 ;0 0 . 02 0 . 0 0 . 0 0 . 0 0 . 0 3*0 C .Oi 0 . 0 0 . 0 0 . 0 ____ u . u 0 . 0 _____________ O .G4 l.OOOOOF 00 OlQ 9 . 99998E— 05 0 . 0 1 .0 0 0 0 J E -G 3 0 . 0
3 1 9.9*70C2E-0i r.0'0"C00"fl-«j5 172^0^06-04 0 .0 1 . 0 0 u u u E - 0 3 J . O7 S f .9 9 0 0 2 c -0 i 2 .1 0 0 0 0 E -0 3 2 .3 0 0 0 0 E -0 4 0 . 0 1 .0 0 0 0 0 E -0 3 C .O"5 g.vannjF-iTI STTTTTIriTrrfKTn mtZCTOT'CTTi n ™ l '.nnt- n.ni ” " 4 . W o 0 2 e - ( ) l '3.0<Jo6tfE-03 " T .6 4 S 9 S E - -3 3 S'.o 4 9 .9 9 0 0 2 F -0 1 2 .0 0 0 0 0 E - 0 3 4 .0 5 9 9 9 E -0 3 0 . 0
l.v iOuOtit -03 0 . 0 1 .0 0 0 0 0 E -0 3 0 . 0
SCATTER iNG MATRIX
ZONE GRP TO GRP 1 2 3 4i l
20 .02 . 00O0QE-O4
1 .1 0 0 0 C E -0 20 . 0
5 . 0 t t 6 0 £ - 0 4 1 .6 0 0 0 0 E - 1 2
2.5 0 Q 0 0 E— 04 5 .0 0 0 0 0 E — 04
34
1 . 0 0 0 0 0 E -0 4 0 .0
2 . 0 0 0 0 0 E -0 40 . 0
0 . 00 . 0
2 . 20000E— 02 C .O
2 1 0 . 0 0 . 0 0 . 0 0 . 0i3
0 . 00 .0
0 . 0O .n
0 . 00 . 0
0 . 6O.v*
4 0 . 0 0 . 0 0 . 0 0 . 0
1 O .C 5 .0 0 0 0 0 E -0 4 3 .0 0 0 0 0 E -0 4 2 .0 0 0 0 0 E -0 42 4 . 0 0 0 0 0E-04 0 . 0 L .3 0 0 0 0 E -0 3 4 .U U O G O E-0 4
3 OOtfGOfc-^ 6 .03 *006 -04 3 .0 l.jaO O ttc-O S » 2Tgi?P§ft£~g4 M.OOOQfte-O _i.QtCgQS-03 J»C,___ 2 - 0 cage *»€R tt»gEO TO CHECK PERTURBATION O E S U t T . 0 1 1 .1 8 O-ANvEO - o0i> ______
W 2 4 S 4 GRGU?\ 864 F O T S fS STREAM OF C i f AT ICK CASiS QftNt 72L IN E *SLAXATtGM WILL #6 UONE CM ROrfS - I JNN£(L IT E R A T IO N !S tI 'AilJJ' . -VV «%iU" ' K ^ ' ,g“" -j^-gV"" ■■■ .^ a -r - — . ^ . r '" J ' J ■ 1 -IffftftTIOK f Llfli CHANGE liEU MU-1 *0-2 »0-3 K
1 T ?,. X} ,<m£-oi i.twaoo -i.44&9i> 0..0 0.0 , o.cvviO]' ................. . .2 4,5?£tSE 00 1.76WW -i.?4»n - 1. r»v5j 0.50454 1712773 3t>4ssae t»o 1*63593 4.32375 ... -0,U63fe ... ..d«.UL4.tS. ........ _______ _ ............ -4 5.T8T37E 00 1*54713 7.41834 a,*1535 -0.Q9CB9 0.1732Y?S oi I.S9717 13.52540 0.22 87 2.728ft. 6.X1b71‘* . . —
■J 6 " " r r s a s r s r g r lATs?69 27.03925 p.Masi ,0k. 111* 5T 2.«)H5et 00 i.4»3*ti v/u 0.1769918 «4*j9$rjf4E-css 1. *fS« - 0.81*07 -0.20175 0.88230 0.178974
-■»- ‘ -5.O1S89E-01 1.47186 0.29506 0.61423 0.70271 0.18024810 -3.277036-01 1.47088 0. 32563 0.72184 0.82827 0.181300u - I .692476-01 1.47042 0.34722 0.80702 0,83967 0.182176ti -1.884686-01 1.47020 0.92510 0.84388 0.85158 0.18294213 -2.001006-01 1.47010 0.86162 0.84107 0.83973 0.183U9914 -U06852E-01 1.47005 0.42714 0.84571 0.83542 0. 18415-.15 -8.6B902E-02 1.47003 0. 72629 0.84523 0.8*3 77 0.18461316 -7.97650E-02 1.47002 0.83823 0.83727 0.84320 0.18500817 -7.55096E-*J2 1*47001 0.87114 0.84042 0.84155 0.185336lA -?.67is5fe-fli i.4?ddi 0.B6646 0.&387& 0.84323 0.18561219 -6.57786E-02 1.47001 0.86370 0.83614 0.84168
-3.98f3«-bl EXTRAPOLATION WITH 5,6630 0.18/14920 3.54176E-02 1.00000 -0. 50302 -3.41471 5.62257 0.187138a -2.t5niE-02 1.47001 -0.80603 -0.70184 -0.00802 0.18711022 -2.672276-02 1.47001 0.94251 0.E3242 1.05322 0.18708423 i29E-d2 1.47601 1.06 1 0.85574 1.05981 0.18706024 -3.1*0226-02 1.470P1 1.26177 1.41054 0.98706 0.18704125 4.8*3^6-62 1.47001 -1.23704 -0.59549 1.18399 0.18701826 2.97499E-02 1.47001 0.64021 1.45*15 0.97594 0.18699527 -2.9*6856-02 1.47001 -1.03039 -0.81784 0.87702 0.18697928 3.20702E-02 1.47001 -1.0452 5 -0.498S9 1.13916 0.13695629 -r.4i5aT?e-02- 1.4t66l -0.45 01 -l.lcld4 6.74414 O.i8694230 8.025176-03 1.47001 -0.55958 -0.07140 1.05163 0.18692631 5.39017E-03 1.4*001 0.67705 0.84535 0.87768 0.18691332 5.00107E-03 1.47001 0.93281 0.83S95 0. 90440 0.1869013J 4.79126E-03 1.4?001 0.96284 0.84223 0.89562 0.18689034 4 . 131326-03 1.47001 0.86639 0.84113 0.88263 0.18688135 3.75462E-03 1.4?66l 0. 91257 0.83784 6.8*814 0.18687336 3.43227E-03 1.47001 0.91758 0.83-330 0.87231 0.18686637 3.071786-P3 1.47C01 0.89604 0.83401 0.86680 0.18686038 2.733236-03 1.47001 0.89252 0.84968 0.86163 0.18685539 2.40803E-03 1.4t00l 0.84343 0.84411 0.85662 0.18685140 2.105716-03 1.47001 0.87656 0.34032 0.85164 0.18684741 1.82915E-03 1.47001 0.8*049 0.8 43 0.84671
1.054456-02 EXTRAPOLATION WITH 5.7753 0.18682742 1.1*46*6-64 1.00000 0.06216 0.55457 5.64097 0 .1 8 6 8 2 743 9 .9 1 & 2 1 E -0 5 1.47001 0 .8 7 4 0 5 1 .5 6 7 5 2 - 0 . 0 1 4 5 i 0 .1 8 6 8 2 744 -7 . 7 9 6 2 9 E - 0 5 1.47001 -0 .7 8 6 1 4 —0 .8 0 6 8 6 1 .2 9 6 7 7 0.1 8 6 8 2 7
END OF EIGENVALUE CALCULATION - ITER A TIO N TIME 0 .0 ? 9 MINUTES
CONVERGENCE IN D ICA TIO N 8V M IN IM IZ IN G THE SUM OF Th E SOUARES OF THE RESIOUES - R E L A T IV E ABSORPTION 1 .0 0 0 0 2 0 0 K 0 .1 8 6 8 3 0 3
LEAKAGE 5 .5 4 2 9 5 E -0 1 TOTAL LOSSES 5 .3 5 2 5 3 E 00 TOTAL PRODUCTIONS l.OOOOOE 00 REACTOR POWERCWAtrSI l.OOOOOE 06
I GROSS NEUTRON BALANCE
GRP1
LFT LEAKAGE 0 . 0
TOP LEAKAGE 1 .0 8 1 0 8 E-0 2
R I T LEAKAGE 2 .9 9 7 8 6 E -D 1
B0T LEAKAGE 0 .0
FNT LEAKAGE 0 .0
BAK LEAKAGE 0 . 0
B**2 LOSSES 4 . 03370E— 02
l / V LOSS 0 . 0
XENON LOSS 0 . 0
23
0 . 00 . 0
5 .0 5 6 3 4 E -0 3 1 .9 8 7 5 5 E -0 3
1 .4 0 2 2 8 E -0 1 5 .4 7 4 2 7 E - 0 2
0 .00 .0
0 . 00 .0
0 . 00 .0
1 . 96899E— 02 7 .62 1 1 8 E— 03
0 . 00 . 0
0 .00 . 0
4 0 . 0 2 .2 3248E-03 3.9 4 5 2 I E - 0 2 0 .0 0 . 0 0 .0 5 .6 8 8 3 8 E— 03 0 . 0 0 . 0
SUM 0 .0 2 .0 0 8 726-02 5 .3 4 2 Q8E-01 0 .0 0 .0 0 .0 7 . 33363E— 02 0 . 0 0 . 0
GRP ABSORPTIONS OUT-SCATTER SOURCE IN -S C A T TE R TOTAL LOSSES TOTAL GAINS PROD/ABSCRP12
2.0 3 6 9 8 E 00 1 . 15671E 00
8 . 33394E-01 5 . 2 9 4 96E-01
3 . 2 U 5 2 E 00 1 .07051E 00
9 . 7 9 4 2 2 E-0 3 7 .B 0 6 7 7 E -0 1
3 .2 2 1 3 1 E 00 1 .8 5 1 1 8 E 00
3 .2 2 1 3 1 E 00 1.85118E 00
1 .3 7 8 1 4E—01 2 .1 5 7 2 3 E -0 1
34
7 .4 0 6 6 2 E -0 1 7 .9 0 5 4 1 E —01
2 .7 3 5 C 7 E -0 12 .3 2 7 4 0 E -0 3
5 .3 5 2 5 3 E -0 15 .3 5 2 5 3 E -0 1
5 .4 3 2 6 8 E—01 3 .0 4 9 8 7 E -0 1
1 .0 7 8 5 2 E 00 8 .4 0 2 4 1 E -0 1
1.07852E 00 8 .4 0 2 4 0 E -0 1
1 .6 2 6 9 2 E — 01 4 .4 1 7 8 0 E -0 L
SUM 4 .7 2 4 8 9 E 00 1 . 6 3 8 72E 00 5.3 5 2 5 3 E 00 1 .6 3 8 72B 00 6 .9 9 1 2 5 E OC 6 .9 9 1 2 5 E 00
GROUP NEUTRON BALANCE FOR EACH ZONE
ZONE NUMBER 1— CORE VOLUME 5. 64858E 04
GRP’ ABSORPTIONS O UT-S C A TTER B**2 LOSSES l / V LOSS XENON LOSS IN -S C A TTE R SOURCE POWER!WATTSi AVERAGE FLUX
CM 1.96508E 00 1 .1 2 2 8 8 E 00
8 .2 4 6 3 2 E -0 15 .2 0 8 9 J E -0 1
3 .1 5 8 3 6 E -0 21 .5 5 9 6 4 E -0 2
0 .00 .0
0 . 00 .0
7 .4 4 3 2 2 E -0 37 .7 4 4 0 6 E -0 1
3.2 1 1 5 2 E1 .07051E
0000
2 .8 0 7 2 6 E 05 2 .4 9 5 2 9 E 05
1 .2 4 2 4 6 E -0 3 5 .5 2 1 9 4 E —04
34
7 .2 2 9 9 9 E -0 17 .8 5 8 0 0 E -0 1
2 .6 8715E-01 0 .0
6 .0 2 5 2 9 E -0 3 4 . 365 8 1 E-0 3
0 .00 .0
0 . 00 . 0
5 .3 * 1 49E-01 2 .9 8 2 4 1 E —01
5 . 35253E— 01 5 . 35253E— 01
1 .2 0 5 0 0 E 05 3 .4 9 2 4 5 E 05
2 .1 3 3 2 8 E — 04 1 .5 4 5 7 2 E -0 4
SUM 4.59 6 7 6 E 00 1 .61424E 00 5 .7 5 7 1 I E - 0 2 0 .0 0 . 0 1.61424E 00 5 .3 5 2 5 3 E 00 9 .9 9 9 9 9 E 05
ZONE NUMBER 2— REFLECTOR VOLUME 4 . 42336E 03
GRP ABSORPTIONS O U T-S CA TTER B**2 LOSSES l / V LOSS XENON LOSS IN -S C A TTE R SOURCE POWER!WATTS) AVERAGE FLUX12
7 .0 8 0 9 5 E -0 23 .2 8 8 9 6 E -0 2
0 .00.0
0.00 . 0
0 .00 .0
0 . 00 . 0 -
0 .00 .0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
34
1 .2 7 9 1 3 E -0 21 .6 0 0 3 8 E -0 5
0 . 00 . 0
0 . 01 .6 0 0 3 8 E -0 4
0 .00 .0
0 . 00 . 0
0 .00 .0
0 . 00 . 0
0 . 00 . 0
0 . 03 . 6 1 8 0 2 E-0 5
SUM 1 . 16506E-01 0 .0 1 .6 0 0 3 8 E -0 4 0 .0 0.0 0 . 0 0 . 0 0 . 0
ZONE NUMBER 3— VOLUME 7. 1980I E 04
GRP ABSORPTIONS O UT-SCATTER 8**2 LOSSES l / V LOSS XENON LOSS IN -S C A TTE R SOURCE POWER!WATTS) AVERAGE FLUX12
1 .0 9 5 2 6 E -0 3 9 .4 2 4 3 9 E— 04
8 .7 6 2 0 8 E -0 3 8 .6 0 4 8 8 E — 03
8. 7 5333E-03 4 .0 9 3 4 7 E -0 3
0 .00 .0
0 .00 . 0
2 .3 5 1 0 1 E -0 3 6 .2 7048E-03
0 . 00 . 0
0 . 0U .O
1.2 1 7 2 9 E—0 4 5 .6 9 2 6 3 E -0 5
34
4 . 8 7230E-03 4 . 7 2460E-03
4 .7 9 2 4 4 E -0 32 .3 2 7 4 0 E -0 3
I .5 9 5 8 9 E -0 3 1 . 16254E-03
0 .00 .0
0 . 00 .0
9 .1 1 9 1 4 E -0 36 .7 4 6 1 4 E -0 3
0 . 00 . 0
0 . 0O .C
2 .2 1 9 3 4 E -0 51 .6 1 6 6 9 E -0 5
SUM 1 .1 6 3 4 6 E -0 2 2 .4 4 8 6 8 E -0 2 1 .5 6 0 5 2 F -0 2 0 .0 0 . 0 2 .4 4 8 6 8 E -0 2 0 . 0 0 . 0
END OF CASE - TOTAL CPU TIME WAS 0 .0 9 MINUTES TCTAL CLOCK TIM E WAS 0 .4 6 MINUTES*************************************************************************************************************** ***************************************************************************************************************
*********t h i s job was run on 03- 11-7 2 on the ibm 360/91*********
2 - 0 CASE PERTURBED T O CHECK PERTURBA TIO N R E S U LT. D < 1 .11 CHANGED - . 2 5 9X24X4 GROUP, 864 PO IN TS STREAM OF C I T A T I O N CASES ORNL 72
F IS S IO N SOURCE D IS T R IB U T IO N AND SUM 0 .6 0 0 0 0 0 .2 0 0 0 0 0 .1 0 0 0 0 0 .1 0 0 0 0 1 .0 0 0 0 0
CORE STORAGE DIFFERENCE (WORDS) EQUATION'CONSTANTS I/ O INSTEAD OF STOREO 1395
EQUATION CONSTANTS WILL BE $TORED IN CORE
NUMBER OF-------COLUMNS. ROWS, PLANES, GROUPS, UPSCAT, DOWNSCAT, REGIONS, AND ZONES 9 24 1 4 3 3 12 3
MEMORY LOCATIONS R C S ER vEd "f6 r 6A?A St6*AGE------ 40000MEMORY LOCATIONS USED FOR T H IS PROBLEM---------------- 7779______________________________________________________________________________________MEMORY LOCATIONS NOT USED-----------■-------------------------------------- 32221
ZONE MACROSCOPIC CROSS SECTIONS
ZONE NAME GRP D SlGR S T g S NUSIGF ‘ BSQ POWEK/FLUXI CORE______________ 1 2 .5 0 0 1 4 E -0 1 1 . I 7 5 0 0 E - 0 2 2 .8 0 0 0 0 E -0 2 4 .0 0 0 0 0 E -0 3 1 .0 0 0 0 0 E -0 3 4 .0 0 0 0 0 E 03
2 5 .0 0 0 2 8 E -0 1 1 .6 7 0 0 0 E -0 2 3 .6 0 0 0 0 E -0 2 8 .0 0 0 0 0 E -0 3 1 .0 0 0 0 0 E -0 3 8 .0 0 0 0 0 E 03____________________________3 5 .0 0 0 2 5 E -0 1 2 .2 3 0 0 0 E - 0 2 5 .9 9 9 9 9 E -0 2 1 .0 0 0 0 0 E -0 2 1 .0 0 0 0 0 E -0 3 l.OOOOOE 04
4 5 .0 0 0 2 8 E -0 1 0 .0 8 .9 9 9 9 9 E -0 2 4 .0 0 0 0 C E -C 2 1 .0 0 0 C 0 E -0 3 4 .0 0 0 0 0 E 04
2 REFLECTOR I 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0_________________________2 0 .0 _______________ 0 .0 ____________ 0±0_______________OiO_____________CM)_______________0 .0
3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0_________________________4 l.OOOOOE 00 0 .0 ____________ 9. 9 9 9 9 8 E -0 5 0 . 0 _____________1 .0 0 0 0 0 E -0 3 0 . 0
3_______________________ 1 9 .9 9 0 0 2 E —01 I . 0 0 0 0 0 E -0 3 1 .2 S 0 0 0 E -0 4 0 . 0 ______________I .O O 0 0 0 E -0 3 0 . 02 9 .9 9 0 0 2 E -0 1 2 .1 0 0 0 0 E - 0 3 2 .3 0 0 0 0 E -0 4 0 . 0 1 .0 0 0 0 0 E -0 3 0 . 0
_____________________________ 3 9 .9 9 0 0 2 E —01 3 .0 0 0 0 0 E - 0 3 3 .0 4 9 9 9 E -0 3 0 . 0 ______________ 1 .0 0 0 0 0 E -0 3 0 .04 9 .9 9 0 P 2 E -0 1 2 .0 0 0 9 0 E -0 3 4 .0 5 9 9 9 E -0 3 0 . 0 1 .0 0 0 0 0 E -0 3 0 . 0
SCATTERING MATRIX--------------------------------------------------------------------------------------------------------------------------------------------------------------------------- ----------------------
ZONE GRP fo Grp i 2 3 41 1 0 .0 1 .1 0 0 0 0 E -0 2 5 .0 C C 0 0 E -0 4 2 . 50000E— 04
2 2 . 0 0 0 O O E-04 0 . 0 1 .6 0 0 0 0 E -0 2 5 .0 0 0 0 0 E -0 43 1 .0 0 0 0 0 E -0 4 2 .0 0 0 0 0 E — 04 0 . 0 2 .2 0 0 0 0 E — 024 0 , 6 0 . 0 0 . 6 0 .0
2 1 0 . 0 0 . 0 0 „0 0 .02 0 . 0 0 . 0 0 . 0 0 .03 0 . 0 0 . 0 0 . 0 0 .04 0 . 0 0 . 0 0 . 0 0 .0
3 1 0 .0 5 .0 0 0 0 0 E - 0 4 3 .0 0 0 0 0 E —04 2 .0 0 0 0 0 E— 042 4 . 0 0 0 00 E-0 4 0 . 0 1* 30 000E—03 4 .0 0 0 0 0 E — 043 3 .0 0 0 0 0 E - 0 4 6 . 0 0 0 0OE-O4 0 . 0 2 . 10000E-034 2 .0 0 0 0 0 E -0 4 8 .0 0 0 0 0 E - 0 4 l . O C 000E -0 3 oTo
2 - 0 CASF PERTURBED TO CHECK PERTURBATION R E S U L T . 0 1 1 .1 1 OAM GED - . 2 5 9X24X4 GROUP, 864 P O IN TS -• STREAM OF C IT A T IO N CASES ORNL 72
L IN E RELAXATION H IL L BE DONE ON ROWS - 1 INNER I T E R A T I O N S ) ______________IT E R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 — 7 . 2 3477E-01 1 .0 0 00 0 - 1 . 4 4 6 9 5 0 . 0 0 . 0 0 .0 9 9 2 8 52 5 .15432E 00 1 .7 6 9 9 3 -1 . 9 7 0 0 5 -1 . 9 7 0 0 5 0 .5 8 1 3 7 0 .1 7 1 6 8 33 3 .5 0 2 0 4 E 00 1 .6 2 5 9 3 4 .1 8 1 4 8 0 .1 0 7 6 8 -0 .0 0 3 6 3 0 .1 7 4 4 3 44 6 .6 5 6 9 9 E 00 1 .54713 8 .5 5 7 8 8 0 . 22383 - 1 1 .3 2 9 6 0 0 .1 7 7 1 5 85 1.28672E 01 1 .5 0 7 1 7 1 4 .8 0 0 0 7 0 .2 0 6 3 7 0 .9 8 9 9 5 0 .1 8 0 9 4 66 2 .7 5 3 2 9 E 01 1 .4 8 7 6 9 29.67271 0 .0 9 5 0 7 0 .4 2 3 8 3 0 .1 8 0 0 9 27 3 .36094E 00 1 .4 7 8 3 6 3.48301 0 .4 5 0 0 0 2 .3 0 4 3 3 0 .1 8 1 7 2 98 - 5 . 1 9 4 5 8E-01 1 .4 7 3 9 4 -0 . 6 7 4 0 2 - 0 . 1 2 6 1 9 0 .8 4 7 9 3 0 .1 8 3 4 0 49 - 5 . 0 7 0 0 1 E - 0 1 1.4 7 1 8 6 0 .46902 0 .5 8 8 8 2 0 .7 7 0 7 5 0 .1 8 4 5 9 8
10 - 2 . 7 2 3 8 0 E - 0 ] 1 .4 7 0 8 8 0 .2 6 4 8 6 0 .7 6 4 9 2 0 .8 4 6 5 5 0.1 8 5 6 4 111 - 1 . 6 2 9 7 9 E - 0 1 1.47042 0 .4 3 5 3 7 0 .8 3 4 6 4 0 .8 3 3 0 4 0 .1 8 6 5 0 8! 2 - 1 . 7 8 8 1 6 E - 0 1 1 .4 7 0 2 0 0 .9 1 8 3 5 0 .8 4 5 6 1 0 .8 4 3 4 7 0 .1 8 7 2 5 913 -1 . 9 8 8 6 1 E - 0 1 1 .4 7 0 1 0 0 .9 1 3 2 4 0 . 86371 0 .8 3 7 2 6 0 .1 8 7 8 9 714 - 1 . 0 3 1 76E-01 1.4 7 0 0 5 0 .4 1 5 6 6 0 . 84771 0.B 3 7 12 0 .1 8 8 4 3 615 — 8 .74956E— 02 1.470C3 0 . 7605 3 0 .8 4 5 1 6 0 .8 4 3 3 9 0 .1 8 8 8 8 516 - 8 . 4 4 4 4 5 E -0 2 1.47002 0 .8 8 0 6 8 0 .8 4 1 1 4 0 .8 4 3 5 2 0 .1 8 9 2 7 117 - 7 . 9 3 9 3 5 E - 0 2 1.47001 0 .8 6 0 7 9 0 .8 3 9 2 2 0 .8 4 2 1 4 0 .1 8 9 5 9 316 - 7 . 4 6 7 3 3 E - C 2 1.47001 0 .8 6 5 8 7 0 .8 4 0 4 8 0 .8 4 3 3 9 0 .1 8 9 8 6 419 -6 . 9 6 9 3 0 E - 0 2 1.47001 0 .86361 0 .8 4 2 6 0 0 .8 4 2 8 6
-4 .3 5 0 6 7 E - 0 1 EXTRAPOLATION WITH 5 .8 0 7 6 0 .1 9 1 4 1 120 3 .5 1 2 2 9 E -0 2 1 .00000 - 0 . 4 6 8 8 4 - 3 . 3 0 2 3 7 5 .7 6 1 3 2 0 .1 9 1 4 0 121 -2 . 7 7 5 0 6 E - 0 2 1.47001 - 0 . 8 1 7 8 5 - 0 . 6 3 775 -0 . 0 1 0 9 6 0 .1 9 1 3 7 522 — 2 .7 0 0 3 2 E -0 2 1.47001 0 .9 4 6 0 6 0. 82868 0.9 6 0 3 7 0 .1 9 1 3 5 0i'i - i . 9 S 6 4 l t - 0 2 1.4 7001 1 .0 6 5 2 7 0 .8 8 8 9 7 0.9 4 1 8 2 0.1 9 1 3 2 824 -3 . 8 5 3 0 0 E - 0 2 1.47001 1 .2 6 4 7 4 1 .4 7 5 43 0.9 2 5 3 7 0 .1 9 1 3 0 925 4 .8 9 1 8 7 E - 0 2 1.4 7 0 0 1 - 1 .2 2 0 7 1 - 0 . 6 1 4 2 7 1.08345 0 .1 9 1 2 8 926 2 .5 9 2 5 6 E -0 2 1.47001 0 .5 5 5 9 0 1 .5 6 1 8 0 0.9 4 2 9 7 0 .1 9 1 2 6 9t't — 3 . 18609E-C2 1.47r*f>l - 1 . 2 6 0 8 0 - 0 . 6 9 7 1 9 0 .9 1 1 4 4 0 .1 9 1 2 5 428 3 .3 3 5 9 5 E -0 2 1.47001 - I . 013t>7 - 0 . 5 8 6 2 5 1.06529 0.1 9 1 2 3 529 - 1 . ^ 6 6 4 6 ^ - 6 ? 1.4*001 - 0 . 5 2 8 6 0 - 0 . 9 9 1 5 6 0 .7 8 8 8 2 0 .1 9 1 2 2 230 1 .O 3 5 3 1 E -0 2 1.470C1 - 0 . 5 9 6 3 5 - 0 . 0 7 7 6 5 1.0 1 5 9 5 0 .1 9 1 2 0 831 5 .1 7 8 4 5 E -0 3 1.47001 0 . 50536 0 .8 4 8 1 6 0 .8 7 9 0 0 0 .1 9 1 1 9 632 4 .7 1 1 1 5 E -0 3 1.47001 0 .9 1 4 4 7 0 .8 4 5 8 7 0 .9 1 4 6 5 0 .1 9 1 1 8 533 '♦•5P325E-03 1.47001 0 .9 6 0 3 7 0 . 850C9 0 .8 9 5 5 0 0 .1 9 1 1 7 534 4 .0 7 8 8 7 6 -0 ? 1.47001 0 .9 0 9 8 4 0 .8 4 3 3 7 0 .8 8 7 5 2 0 .1 9 1 1 6 735 1.4 7001 0 .9 2 4 4 9 0 .8 4 6 2 8 0 .8 8 3 8 5 0 .1 9 1 1 5 936 3 .4 8 6 6 3 E -0 3 1.47001 0 .9 3 1 8 8 0 .8 4 3 9 7 C . 87746 0 .1 9 1 1 5 33? 3 .1 6 1 4 3 F -0 3 1.47001 0 .9 0 9 8 9 0 .8 4 1 2 7 0.8 7 2 7 7 0 .1 9 1 1 4 738 2 .8 6 1 9 B E -0 ? 1.47001 0 .9 0 8 1 4 0 .8 3 7 7 4 0 .8 6 8 1 9 0 .1 9 1 1 4 239 S .5 5 6 B 0 E -0 3 1.47001 0 .8 9 5 9 3 0 .8 3 4 6 8 0 .8 6 3 4 8 0.1 9 1 1 3 840 2 .2 6 8 7 9 E -0 3 1.47001 Oo88962 0 .8 3 7 9 6 0 .8 5 9 2 7 0 .1 9 1 1 3 4
--4 1 1.49795E-63 1.47001 0. 88 16 2 0 .8 4 8 1 0 0 .8 5 4 7 31 .2 8 1 5 8 E -0 2 EXTRAPOLATION WITH 6 .4271 0 .1 9 1 1 1 2
42 1 .1 7 3 0 2 E -0 4 1 .0 0 0 0 0 0 .0 5 8 8 3 0 .6 7 6 8 6 6 .2 7 4 3 1 0 .1 9 1 1 1 243 - 1 . 0 2 1 6 2 E - 0 4 1.47001 - 0 . 6 7 1 0 4 —1•45 56 9 -0 * 0 1 8 3 1 0.1 9 1 1 1 244 - 9 . 9 3 6 0 9 E - 0 5 1.47001 0 .9 7 2 4 8 0 .5 4 7 2 3 1.1 4 0 2 6 0 .1 9 1 1 1 3
END O F EIGENVALUE CALCULATION - H h R A IlU N 11Mb O .C81 MifcOTES
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM Of THE SQUARES OF THE RESIDUES - R E L A T IV E ABSORPTION 1 .0 0 0 0 1 9 1 K 0 .1 9 1 1 1 5 7
LEAKAGE 4 .4 9 8 1 9 E —01 TOTAL LOSSES 5 .2 3 2 5 1 E 00 TO TAL PRODUCTIONS l.OOOOOE 00 REACTOR POHERIWATTS) l.OOOOOE 06
CROSS NfrUTROto BAl ANCF
GBPI
L F T LEAKAGF 0 . 0
TOP L6AKAGE 7 .1 2 7 2 3 6 -0 3
K I T LEAKAGE 2 . 131 4 9 E-0 1
BOT LEAKAGE C.O
FNT LEAKAGE 0 .0
BAK LEAKAGE 0 .0
B**2 LOSSES 2 .4 1 1 7 0 E - 0 2
1/V LOSS 0 . 0
XENON LOSS 0 . 0
23
0 . 00 . 0
4 .4 6 7 S 5 F -0 31 .7 6 0 6 7 6 -0 3
1 . 32583E-01 5 . 167 4 7 F-0 2
0 .00 .0
0 .00 . 0
0 .00 . 0
1.9 4 6 9 5 E- 7 . 484146-
-02-0 3
0 . 00 . 0
0 . 00 . 0
4 0 . 0 2 .0 0 5 3 9 6 -0 3 3 . 705 0 7 E-0 2 0 .0 0 . 0 0 . 0 5 . 54651E— 03 0 . 0 0 . 0
§UM 0 . 0 1 .5 3 6 1 2 E -0 2 4 .3 4 4 5 8 6 -0 1 0 .0 0 . 0 0 .0 5 .6 6 1 7 2 6 -0 2 0 . 0 0 . 0
GRP ABSORPTIONS OUT— SCATTER SOURCE IN -S C A T T E R TOTAL LOSSES TOTAL GAINS PROD/ABSCRP12
2 .0 5 6 8 1 E 00 1 .1 5 6 0 0 6 00
8 .4 7 9 5 3 5 -0 15 .2 9 2 6 6 F -0 1
3 .1 3 9 5 0 6 00 1 .P4650E 0 0
9 .6 5 5 1 8 6 -0 3 7 .9 5 2 6 8 E —01
3 .1 4 9 1 6 E 00 1 .8 4 1 78E 00
3 .1 4 9 1 6 E 00 1.B417VE 00
1 .3 9 3 1 7 E -0 12 .1 5 9 5 8 6 -0 1
i4
?.3t4i¥Gfe-6t 7 . 7897 9 E-0 1
2 .7 1 1 5 4 E -0 12 .1 8 3 9 3 E -0 3
5 .2 3 2 S 1 E -0 1 5 . 2 3251E-01
5 .4 3 1 0 0 E —01 3 .0 2 5 1 3 6 -0 1
lr 0 6 b 3 S E 00 B .2 5 7 6 5 E —01
1 .0 6 6 3 5 E 00 8 .2 S 7 6 4 E -0 1
1 .6 2 8 3 5 E -0 14 .4 1 9 0 7 E -0 1
SIM 4 .7 2 6 0 7 E CO 1 .6 5 C 5 5 E 00 5 .2 3 2 5 1 6 00 1 .6 5 0 5 5 E 00 6.8tt30b6 00 6 .8 8 3 0 6 E 00
CROUP NEUTRON BALANCE FOR FACH ZONE
ZONE NUMBER 1— CORE VOLUME 5 . 648586 04
CRP ABSORPTIONS O U T-S CA TTER 8**2 LOSSES 1/V LOSS XENON LOSS IN -S C A TTE R SOURCE POhERIWATTS) AVERAGE FLUXt2
z.o o sssi 661 .12 3 4 1 E 00
& .il? 4 6 £ -0 i 5 . 2 1 140E-01
1 .¥ 9 1 0 4 6 -0 2 1 .5 6 0 3 9 E -0 2
0 . 00 .0
0 . 00 . 0
7 .4 3 6 8 5 6 -0 3 7 .9 0 4 0 3 6 -0 1
3 . 13950E 1 .0 4 6 5 0 6
0000
2 .8 6 5 5 0 E2 .4 9 6 4 4 6
0505
1 .2 6 B 24 E—03 5 .5 2 4 5 7 6 -0 4
5 '4
7 .17396E-01 7.74530E-01
2 .6 6 6 3 3 F -U 10 . 0
5 . 978&0E-03 4 .3 0 3 1 9 6 -0 3
0 .00 . 0
u.o0 . 0
5 .3 5 1 1 4 E — 01 2 .9 6 5 5 4 6 -0 1
5 . 23251E- 5 . 2325I E -
01■01
1.19S66E3 .4 4 2 3 6 E
0505
2 . 11675E-Q4 1 . 523 5 5 E-0 4
SIM 4 .6 2 1 1 9 E 00 1 .62951C 00 4 .3 7 9 6 0 6 -0 2 0 .0 0 . 0 1 .6 2 9 5 1 6 00 5 .2 3 2 5 1 6 00 l.OOOOOE 06
ZONE NUKRFR 2— REFLECTOR VOLUME 4 . 423366 03
GRP ABSORPTIONS O U T-S C A TTE R 8**2 LOSSES 1/V LOSS KEKu n LOSS IN -S C A T TE R SOURCE POhERIWATTS) AVERAGE FLUX12
5 .D 1 9 0 1 E -0 23.169656-02
0 .00.0
o.<?0 . 0
0 .00 .0
0 . 00 . 0
0.00 .0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
54
1 .2 2 8 5 3 6 -0 2 1. 5 2 4 4 8 6 -0 5
"ft. 6 0 .0
O .U1 .5 2 4 4 7 6 -0 4
0 . 00 .0
0 . 00 . 0
0 . 00 .0
0 . 0O .C
0 . 00 . 0
0 . 03 .4 4 6 4 2 E —05
SIM 9 .4 1 8 7 0 6 -0 2 o.g 1 .5 2 4 4 7 6 -0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
ZONF NUMBER 3— V0LUM6 7. 19801E 04
GRP ABSORPTIONS O UT-S C A TTER 0**2 L0SS6S 1/V LOSS X6N0N LOSS I N -S C A T TE* SOURCE POhERtWATTS) AVERAGE FLUX12
7 .7 6 6 1 1 6 -0 4 8 .8 9 9 9 3 6 -0 4
6 .2 1 2 8 7 E -0 3 8 . 1 2 6 Cd E -0 3
6 .2 0 6 6 7 E-03 2.86569E—03
0 .00 . 0
0 . 00 . 0
2 .2 1 8 3 3 E -0 34 .8 4 4 2 4 6 -0 3
0 . 00 . 0
0 . 00 . 0
8 .6 3 1 3 8 E —05 3 .3 7 5 8 6 6 —05
34
4 .5 9 6 4 6 E - 0 34 . 4 3 3 3 6 6 -0 3
4 . 5 7 1 14E-03 2 .1 8 3 9 3 E -0 3
1 .5 0 5 5 4 6 -0 3 1 .0 9 0 8 8 6 -0 3
0 .00 .0
0 . 00 . 0
7 .9 8 6 2 4 6 -0 35 .9 5 5 1 9 E -0 3
o.c0 . 0
0 . 00 . 0
2 .0 9 3 7 0 E —05 1 .5 1 7 0 4 E —05
SIM 1 .0 6 9 6 4 6 -0 2 2 . 1 0 4 40E-02 1 .2 6 6 8 8 6 -0 2 0 . 0 0 . 0 2 .1 0 4 4 0 6 -0 2 0 . 0 0 . 0
END OF CASE - TOTAL CPU TIME WAS 0 .1 0 MINUTES TOTAL CLOCK TIME MAS, 0 .4 3 MINUTES
••♦•♦♦♦••THIS JOB HAS RUN ON 0 3 -1 1 -7 2 ON THE IBM 360/91*********
2 - 0 F1KE0 SOURCE PROBLEM C X .Y - NO F IS S IO N SOURCE. AFTER KAPLAN!________39X41X1 GROUP. 1599 POINTS STREAM OF C I T A T I O N CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 - 5 0 0 0 0 0 0 0 0 1 0 0 0 0 01 0 1 1 1 0 0 O i l 0 0 0 0 0 0 0 0 0 0 0 0 0 0
SO 100 10 2 3 0 0 l.SOOOOOE 00 5 .C J 0 0 0 0 E -0 1
0 0 0 9 .9 9 9 9 9 9 E 09
0 0 0 9 .9 9 9 9 9 9 E
023
00 . 0
0 0 0 12 6 l.OOOOOOE
1200
6 12 24
NEUTRON FLUX PROBLEM DESC RIPTIO N - SEC TION 003
O O O Q 6 0 0 0 0 0 1 1 1 1 0 0 0 0 0 0 0 0 0 09.9 9 9 9 9 9 E —05 1 .0 0 0 0 0 0 E -0 5 9 .9 9 9 9 9 9 E -0 5 0 . 0 0 . 0 l.OOOOOOE 00
9 .9 9 9 S 9 9 E —05 l.OOOOOOE 00
9 . 9 9 9 9 9 9 E -0 5 l.OOOOOOE 00
0 . 00 .0
L E F T .T 0 P t R I6 H T .B 0 T T 0 M t F R 0 N T .B A C K BOUNDARY C C N D IT IC N S ARE_______________________________________0 . 0 0 . 0 0 . 0 0 . 0 4 .6 9 2 0 0 0 E —01 4 .6 9 2 0 0 0 E -0 1
TMO OIMENSIONAL SLAB GEOMETRY ( X . Y ) WIDTH 1 .9 0 4 9 9 9 E 01 HEIGHT 1 .904999E 01
RtGIfiN I C A I I O n JPTS REGION WIDTH
2 9 .0 8 7 9 9 9 E -0 1 15 7.7 7 6 0 9 9 E 00 5 1 .6 8 0 2 0 0 E 00 15 7.7 7 6 0 9 9 E 00 2 9 .0 8 7 9 9 VE-0 1
PTS17
Re g i o n riEISHT 8 .8 1 3 8 0 0 E 00 4 1 .4 2 2 4 0 0 E 00 2 2 .8 0 8 9 9 9 E -0 1 15 6.8 2 9 2 0 0 E 00 3 1 .7 0 3 6 9 9 E 00
X—D I R . POINTS 39 Y - O I R . POINTS 41
DISTANCES TO HESH INTERVAL INTERFACES
J D I S T .2 0 .4 5 4 3 0 .9 0 9 4 1 .4 2 7 5 1 .9 4 6 6 2 .4 6 4 7 2 .9 S 2 8 3 .5 0 1 9 4 .0 1 9 10 4 .5 3 8
11 5 .0 5 6 12 5 .5 7 4 13 6 .0 9 3 14 6 .6 1 1 15 7 .1 3 0 16 7 .6 4 8 17 8 .1 6 6 18 8 .6 8 5 19 9 .0 2 120 9 .3 5 7 21 9 .6 9 3 22 1 0 .0 2 9 23 1 0 .3 C 5 24 1 0 .8 8 4 25 1 1 .4 0 2 20 1 1 .9 2 0 27 1 2 .4 3 9 28 1 2 .9 5 729 1 3 .4 7 6 30 1 3 .9 9 4 31 14 .5 1 2 32 1 5 .0 3 1 33 15 .5 4 9 34 1 6 .0 6 8 35 1 6 .5 8 6 36 1 7 .1 0 4 37 17 .6 2 3
" 3ft » . n r 59 1 8 .596 40 19.o50
I DIST.2 o .s ie 3 1 .0 3 7 4 1 .5 5 5 5 2 . 0 7 4 6 2 .5 9 2 **# 3 .1 1 1 8 3 .6 2 9 9 4 .1 4 8 10 4 .6 6 6
11 5 .1 8 5 12 5 .7 0 3 13 6 .2 2 2 14 6 .7 4 0 15 7 .2 5 8 16 7 .7 7 7 17 8 .2 9 5 16 8 .8 1 4 19 9 .1 6 920 9 .5 2 5 21 9 .8 8 1 22 1 0 .2 3 6 23 1 0 .3 7 7 24 10 .5 1 7 25 1 0 .9 7 2 26 11 .4 2 8 27 1 1 .8 8 3 28 1 2 .3 3 829“ 12.743 30 15.244 51 13 .7 0 4 52 T 4 . 154 33 1 4 .6 1 5 34 1 5 .0 7 0 35 1 5 .5 2 5 36 1 5 .9 8 0 37 1 6 .4 3 638 1 6.891 39 1 7 .3 4 6 40 17 .9 1 4 41 1 8 .4 8 2 42 1 9 .0 5 0 ■
DISTANCES TO FLUX POINTS
J DIST.1 6.227 2 0 . 682 5 1.1 6 8 4 176 86 5 2".26i> 6 2:755 1 7 3 .2 4 2 8 3 .7 6 0 9 4 .2 7 8
10 4 .7 9 7 11 5 .3 1 5 12 5 .8 3 4 13 6 .3 5 2 14 6 .8 7 0 15 7 .3 8 9 16 7 .9 0 7 17 8 .4 2 6 18 8 .8 5 39 .1 6 9 2b 21 9 .8 6 1 22 T o . l i t 23 1 0 .6 2 4 24 1 1 .1 4 3 25 1 1 .6 6 1 26 1 2 .1 8 0 27 1 2 .6 9 8
28 1 3 .2 1 6 29 1 3 .7 3 5 30 14 .2 5 3 31 1 4 .7 7 2 32 1 5 .2 9 0 33 1 5 .8 0 8 34 16 .3 2 7 35 1 6 .8 4 5 36 1 7 .3 6 437 1 7 .8 8 2 38 1 8 .3 6 8 39 1 8 .8 2 3
I D I S T .I 0 . 2 5 9 2 0 .7 7 8 3 1 .2 9 6 h 1 .8 1 5 5 2 .3 3 3 6 2 .8 3 2 7 3 .3 7 0 8 3 . 8 3 8 9 4 .4 G 7
10 4 .9 2 5 11 5 . 4 4 4 12 5 .9 6 2 13 6 .4 8 1 14 6 .9 9 9 15 J .5 1 8 16 8*036 17 8 .5 5 5 18 '6 .99219 9 .3 4 7 20 9 .7 0 3 21 1 0 .0 5 8 22 1 0 .3 0 6 23 1 0 .4 4 7 24 1 0 .7 4 5 25 1 1 .2 0 0 2b 1 1 .6 5 5 27 12.11126 1 2 .5 6 6 29 1 3 .0 2 1 30 1 3 .4 7 6 31 1 3 .9 3 2 32 1 4 .3 8 7 33 1 4 .8 4 2 34 1 5 .2 9 8 35 1 5 .7 5 3 36 1 6 .2 0 837 1 6 .6 6 3 38 1 7 .1 1 9 39 1 7 .6 3 0 40 1 8 .1 9 8 41 1 8 .7 6 6 ________________________________________________________________________
ZONE INPUT .BY REGION5 1 5 2 55 5 5 5 55 5 5 3 55 4 5 3 55 5 5 3 5
ZONE NUMBER AT E CH MESH INTERVAL
1 2 5 5 6 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39
1 5 5 1 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 52 5 5 1 1 1 I 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 53 5 5 1 1 1 1 1 1 1 1 I 1 I 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 54 5 5 1 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 55 5 5 1 I 1 1 1 1 1 1 1 1 1 1 1 4 s 4 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 56 5 5 1 1 1 1 1 I I 1 1 1 1 I 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 57 S $ 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 58 5 5 1 1 1 1 1 1 1 1 X 1 I 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 59 5 $ 1 I 1 1 1 1 1 1 1 1 1 i 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 510 5 5 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 511 S $ 1 1 I 1 1 1 i 1 i 1 i 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 5U 5 5 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 513 5 5 1 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 514 5 5 1 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 515 5 5 1 1 1 1 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 516 5 5 1 1 1 1 1 1 1 1 1 1 1 L 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 5T 7 " 5 $ 1 1 1 I 1 1 1 1 1 1 1 1 1 5 5 5 5 5 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 5 518 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 519 5 5 5 S 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 i> 5 5 5 5 5 5 5 5 5 5 t> 5 >20 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 521 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 522 5 5 5 S 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 3 it 3 3 3 3 3 3 3 3 3 3 3 3 3 S 5£3 5 5 5 5 5 5 5 5 5 5 i> 4 5 5 5 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 524 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 525 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 526 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 S 527 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 528 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 529 s 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 530 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 ? 531 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 532 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 533 5 5 4 4 4 4 ' 4 4 4 4 4 4 4 4 4 4 4 5 5 S 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 534 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 5
5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 536 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 $ 537 5 5 4 4 4 4 4 4. 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 538 5 5 4 4 4 4 4 4 4 4 4 4 4 4 4 4 4 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 539 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 540 5 5 s 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 5<!' S 5 5 5 5 4 5 4 $ 5 5 s 4 s 4 5 5 5 5 5 5 5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 5 5
F I& S IO N SOURCE D IS T R IB U T IO N AND SUM 070 oTO
DESC RIPTIO N OF REACTOR 70NPS
ZN TO ZN SU8-ZNS SIGHA— SET 10 CLuSS OPL NEX NAME1 1 0 0 0 0 0 c BLANKET 12 2 0 0 0 0 0 0 BLANKET 23 3 0 0 0 0 0 0 BLANKET 34 4 0 0 0 0 0 p SEED5 5 0 0 0 0 0 0 H0D-S1K
x
F IX E D SOURCE IN P U T SECTION 026
Z ONE- SOURCE(N/CC -S E C I1 2 .1 4 2 3 1 E - 0 3 2 2 .1 5 0 2 4 E -0 3 3 2 . 17 729E— 03 4 1 .0 4 8 C 8 E -0 2
SOURCE D I S T R IB U T IO N AND SUMl.OOOOE 00 1 . OOOOD 00
POINT NEUTRON SOURCE- N/SEC
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10 0 . 0 0 . 0 5 . 75BE— 04 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E —04 5 .7 5 B E -0 4 S .7 5 8 E — 04 5 . 7 5 8 E -0 4 5 .7 5 8 E — 04 5 .7 5 8 E — 0411 0 . 0 0 . 0 5 .7 5 8 F - 0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E — 04 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 . 7 5 8 E— 0412 0 . 0 0 .0 5 . 7 5 B E - 04 5 . 7 5 8 E -0 4 5 .7 5 8 E — 04 5 .7 S S E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 6 - 0 4 5 :.7 5 8 6 -0 413 0 . 0 0 . 0 5 .> 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 J » . 7 5 8 E - C 4 ‘ 5 .7 5 8 6 -0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E — 04 5 .7 5 8 6 —04 5 .7 5 8 E — 0414 0 . 0 0 .0 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 .7 5 8 c —04 5 .7 5 8 E - 0 4 5 « 7 5 8 E -0 4 5 .7 5 B E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E - 0415 0 . 0 0 . 0 5 . 7 5 8 E - 0 4 5 .7 5 8 E —04 5 .7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 . 7 5 8 6 - 0 4 1 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E—0416 0 . 0 0 . 0 5 .7 5 8 E - 0 4 5 . 7 S 8 E - 0 4 5 .7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 S 8 E -0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 . 7 5 3 E - 0417 0.0 0.0 5 . 7 5 8 E -0 4 5 . 7 5 8 E -0 4 5 .7 5 S E -0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 » 758E— 04 5 . 7 5 8 E - 0 4 5 .7 5 8 6 -0 4 5 .7 5 8 5 — 0418 0 . 0 0 .0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 O .C 0 . 019 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 020 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 021 0 . 0 0 .0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 022 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 023 o . c 0 . 0 O .C 0 . 6 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 024 0 . 0 0 .0 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E — 03 2 .4 7 4 E —03 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E -0 3 2 .4 7 4 E — 03
d . o 0.0 2 . 4 74E-03 2. 474E-63 2 .4 / 4 t ! -0 3 T .4 7 4 E -5 3 5 . 4 2 .4 7 4 £ - 0 3 2 .4 7 4 6 -0 3 2 . 4 7 4 6 - 0 3 2 . 4 7 4 E — 032b 0 . 0 0 . 0 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 . 4 7 4 E -0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E -0 327 0 . 0 0 . 0 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E — 03 2 .4 7 4 E —03 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 03 2 .4 7 4 E —03 2 . 4 7 4 E - 0 328 0 . 0 0 . 0 2 . 4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E -0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E -0 3 2 . 4 7 4 E - 0 329 0 . 0 0 . 0 2 .4 7 4 E - 0 3 2 .4 > 4 t -C 3 _ 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E —0330 0 . 0 0 . 0 2 .4 7 4 E - 0 3 2 . 4 7 4 F -0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - Q 3 2 .4 7 4 E - 0 3 2 .4 7 4 6 -0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 2 . 4 7 4 E - 0 3i i 6 . 0 6 . 6 £ .4 7 4 E — 63 1.4T4E-63 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 } 2 .4 > 4 E - 0 3 2 . 4 ? 4 t - 0 3 2 .4 7 4 E — 03 2 .4 7 4 E —03 2 .4 7 4 E - 0 332 0 . 0 3 .0 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E — 03 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3
"S3 6 . 0 6 . 6 2 .4 7 4 £ - d 3 ~ i . 4 7 4 f -0 3 " 2 .4 7 4 E - 0 3 Z . 4 7 4 E - 0 3 2 . 4 H e- 0 3 Z . 4 7 4 t : -0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 . 4 7 4 £ - 0 334 0 . 0 0 . 0 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E — 03 2 . 4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E — 03 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 E -0 355 0 . 0 6 . 0 2 . 4 * 4 6 -6 3 5 . 4 7 4 E - 0 3 2 .4 7 4 E — 03 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 6 -0 336 0 . 0 0 . 0 2 . 4 7 4 E -0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 E — 03 2 .4 7 4 6 — 03 2 . 4 7 4 6 -0 3
■"17 ' 9.0 0 .0 Z.474E-03 £ . 4 J 4 e - 0 3 - 2.*7*F-03 7.474E-63 2.T74E-7T3' "2.474r-(53' 2 . 4 ^ 4 6 - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 6 - 0 338 0 . 0 0 . 0 2 .4 7 4 E — 03 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E -0 3 2 .4 7 4 E — 03 2 .4 7 4 E - 0 3 . 2 .4 7 4 E -0 3
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12 13 14 15 16 17 18 19 20 21 221 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 02 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 03 5 .7 5 8 E - 0 4 S . 75 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 04 5 . 7 5 8 E - 0 4 5 .7 5 8 E -C 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 05 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 6 -0 4 5 .7 5 8 E —04 0 . 0 0 . 0 0 . 0 0 . 0 0 . 06 5 .7 5 8 E - 0 4 5 .7 5 8 E — 04 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 .0 0 . 0 0 . 07 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E —04 5 .7 5 8 E - 0 4 5 .7 5 8 E — 04 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 _8 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 . 7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 09 5 . 7 5 8 E - 0 4 5 .7 5 8 E —04 5 . 7 5 8 E - 0 4 5 . 7 5 8 E - 0 4 5 .7 5 8 E — 04 5 . 7 5 8 E - 0 4 0 . 0 0 . 0 0 .0 0 . 0 . QtO ...... .
10 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 . 7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 011 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5. 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 012 5 . 7 5 8 6 -0 4 5 .7 5 8 E — 04 5 .7 5 8 E - 0 4 5 . 758E— 04 5 .7 5 8 E -0 4 5 .7 5 8 E —04 0 . 0 0 . 0 0 . 0 0 . 0 0 . 013 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E -0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 o . c 0 . 014 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 6 -0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 .0 0 . 0 0 . 015 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -C 4 5 .7 5 8 E -0 4 5 .7 5 8 E - 0 4 0 . 0 0 . 0 0 . 0 0 . 0 0 . 016 5 .7 5 8 E — 04 5 . 75 8 E -0 4 5 .7 5 8 E - 0 4 5 . 7 5 8 E -0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E —04 0 .0 0 . 0 0 .0 0 . 0 0 . 017 5 .7 5 8 E - 0 4 5 .7 5 8 E — 04 5 . 7 5 8 E - 0 4 5 .7 5 8 E - 0 4 5 .7 5 8 E —04 5 .7 5 8 E —04 0 . 0 0 . 0 0 . 0 0 . 0 0 . 016 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 019 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 020 0 . 0 0 .0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 021 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 022 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 023 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0£4 £ .4 Y 4 £ -o & 2 .4 7 4 6 - 6 3 2 . 4 7 4 E - 0 j5 2 . 4 7 4 6 -0 3 2 .4 7 4 E — 03 2 . 4 7 4 E - 0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 025 2 .4 7 4 E - 0 3 2 .4 7 4 E -0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 _26 2 .4 7 4 E - 0 3 2 .4 7 4 6 -0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E -0 3 2 .4 7 4 6 -0 3 0 . 0 0 . 0 0 .0 o . c 0 . 027 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 6 -0 3 2 .4 7 4 6 -0 3 0 . 0 0 . 0 0 .0 0 . 0 0 . 0
~2a 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 6 -0 3 2 .4 7 4 E —03 0 . 0 0 . 0 0 . 0 0 . 0 0 . 029 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 , 4 7 4 E -0 3 2 .4 7 4 E -0 3 2 . 4 7 4 6 -0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 030 2 .4 * 4 6 -6 4 2 . 4 ? 4 6 -6 5 2 .4 * 4 6 -0 3 2 .4 7 4 E —03 2 .4 7 4 6 -0 3 2 . 4 / 4 6 -0 3 0 . 0 0 . 0 0 .0 0 . 0 0 . 031 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E -0 3 2 .4 7 4 6 -0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 032 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 6 -0 3 2 . 4 7 4 6 -0 3 2 . 4 7 4 6 - 0 3 0 . 0 0 . 0 0 .0 0 . 0 0 . 033 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 E - 0 3 2 .4 7 4 E —03 2 .4 7 4 6 — O i 2 . 4 7 4 6 - 0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0 ....34 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 c - 0 3 2 .4 7 4 6 -0 3 2 .4 7 4 E -0 3 2 .4 7 4 6 -0 3 0 . 0 0 . 0 0 .0 0 . 0 0 . 035 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E —03 0 . 0 0 . 0 0 . 0 0 . 0 0 . 056 2 . 4 7 4 P - C 3 ' 2 .4 T 4 E -6 3 2 .4 7 4 E - 6 3 2 .4 > 4 E - 0 3 2 .4 7 4 6 -6 3 2 .4 7 4 6 - 0 3 6 . 0 0 . 0 0 . 0 0 . 0 0 . 037 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 038 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 .4 7 4 E - 0 3 2 . 4 7 4 E - 0 3 2 .4 7 4 E - 0 3 0 . 0 0 . 0 0 . 0 0 . 0 0 . 039 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 . 040 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 . 041 0 . 0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0 0 . 0 0 .0 0 . 0 0 . 0
23 24 25 26 27 28 29 30 31 32 331 5 .7 7 9 E — 04 5 .7 7 9 E - 0 4 5 . 7 7 9 E - 0 4 5 . 7 7 9 E - 0 4 5 .7 7 9 E -0 4 5 . 7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 .7 7 9 6 — 04 5 . 7 7 9 E -0 4 5 . 7 7 9 E - 0 4 5 . 7 7 9 6 - 0 42 5-»779E— 04 5 .7 7 9 E -C 4 5 . 7 7 9 E -0 4 5 . 7 7 9 E - 0 4 5 .7 7 9 E - 0 4 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 .7 7 9 E - 0 4 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 . 7 7 9 E -0 43 5 .7 7 9 E - 0 4 5 . 7 7 9 E - 0 4 5 .7 7 9 E - 0 4 5 . 7 7 9 E - 0 4 5 .7 * 9 E -0 4 5 .7 7 9 E —04 5 . 7 7 9 E -0 4 5 .7 7 9 E - 0 4 5 .7 7 9 E -U 4 5 . 7 7 9 E -0 4 5 . 7 7 9 E -0 44 5 . 7 7 9 E - 0 4 5 .7 7 9 E —04 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 . 7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 .7 7 9 E - 0 4 5 .7 7 9 E - 0 4 5 .7 7 9 6 -0 4 5 . 7 7 9 6 -0 4 5 . 7 7 9 E -0 45 S . 7 t 9 E - 0 4 $ .7 7 9 E - 0 4 5 . 7'79E-04 5 .7 7 9 6 -0 4 5 . 7 7 9 6 -0 4 5 .7 7 9 £ -0 4 5 . 7 79E-04 5 . 7 7 9 6 -0 4 5 . 7 7 9 6 -0 4 5 . 7 7 9 E -0 46 5 . 7 7 9 E - 0 4 5 .7 7 9 E —04 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 .7 7 9 E -0 4 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 .7 7 9 E — 04 5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4 5 . 7 7 9 E -0 4
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5 .1 3 9 E - 0 4 5 .1 3 9 E — 04
5 .1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E—04 5 .1 3 9 6 -0 4
2930
5 . 1 3 9 E - 0 4 5 . 1 39E—04
5 . 1 3 9 E -0 4 5 . 1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E - 0 45 .1 3 V E -0 4
5 . 1 3 9 E - 0 4 5 . 1 3 9 E -0 4
5 . 1 3 9 6 - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 .1 3 9 E - 0 4 5 .1 3 9 E —04
5 . 1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 .1 3 9 E —04 5 . 1 3 9 E - 0 4
3132
5 . I 3 9 E - 0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E-04
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E -0 45 .1 3 9 E - 0 4
5 . 1 3 9 6 - 0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E - 0 4 5 . I 3 9 t — 04
5 . 1 3 9 6 - 0 4 . 5 . 1 3 9 E - 0 4
5 .1 3 9 6 -0 45 . 1 3 9 6 - 0 4
3334
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1?9E— 04
5 .1 3 9 E — 04 5 .1 3 9 E — 04
5 . 1 3 9 E - 0 45 . 1 3 9 6 -0 4
5 .1 3 9 6 -0 45 .1 3 9 6 - 0 4
3536
5 . 1 3 9 E -0 4 5 .1 3 9 F -0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E - 0 4
5 . 1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E - 0 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E — 04 5 .1 3 9 E — 04
5 . 1 3 9 E -0 4 . 5 .1 3 9 E - 0 4
5 . 1 3 9 E - 04 5 .1 3 9 6 -0 4
3738
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 F -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 .1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 .1 3 9 E — 04 5 .1 3 9 E — 04
5 .1 3 9 E - 0 4 5 . 1 3 9 E -0 4
5 .1 3 9 E — 04 5 .1 3 9 E — 04
5 . 1 3 9 E - 0 45 .1 3 9 E -0 4 *
5 . 1 3 9 6 - 0 45 .1 3 9 6 -0 4
3940
6 .4 1 0 E - 0 46 .4 1 0 E - 0 4
6 . 4 1 0 E - 0 46 .4 1 0 E - 0 4
6 . 4 1 0 E -0 4 6 .4 1 0 E - 0 4
6 . 4 1 0 E - 0 46 . 4 1 0 E - 0 4
6 .4 1 O E -0 46 .4 1 0 E —04
6 .4 1 0 E - Q 46 . 4 1 0 E - 0 4
6 . 4 1 0 E - 0 46 . 4 1 0 E - 0 4
6 .4 1 0 E - 0 4 6 .4 1 0 E — 04
6 .4 1 0 E - 0 46 . 4 1 0 E - 0 4
6 . 4 1 0 E - 0 4 6 .4 1 0 E —04
6 .4 1 0 £ — 04 6 . 4 1 0 6 - 0 4
41 6 .4 1 0 E - 0 4 6 .4 1 0 E - 0 4 6 . 4 1 0 E - 0 4 6 . 4 1 0 E - 0 4 6 .4 1 0 E - 0 4 6 . 4 1 0 E - 0 4 6 . 4 1 0 E - 0 4 6 .4 1 0 E — 04 6 .4 1 0 E - 0 4 6 .4 1 0 E —04 6 .4 1 0 E — 04
134
5 . 7 7 9 E - 0 435
5 . 7 7 9 E - 0 436
5 . 7 7 9 E - 0 437
5 . 7 7 9 E -0 438
C.O39
0 . 023
5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4
5 .7 7 9 E - 0 4 5 . 779E—04
5 . 7 7 9 E - 0 4 5 . 7 7 9 E -0 4
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
0 .00 .0
0 . 00 . 0
45
5 . 7 7 9 E - 0 4 5 . 7 7 9 E - 04
5 . 779E—04 5 . 7 7 9 E -0 4
5 . 7 7 9 1 - 0 4 5 . 7 7 9 E - 04
5 . 7 7 9 E - 0 45 .7 7 9 E - 0 4
0 .00 .0
0 . 00 . 0
67
5 . 7 7 9 E -0 4 5 .7 7 9 E - 0 4
5 . 7 7 9 E - 0 45 .7 7 9 E - 0 4
5 . 7 7 9 E -0 4 5 . 7 7 9 F -P 4
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
0 .0C.O
O .U0 . 0
89
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
5 .7 7 9 6 -0 4 5 . 77VE— 04
5 . 7 7 9 E - 0 45 . 7 7 9 F - 0 4
5 . 7 7 9 E - 0 4 5 . 7 7 9 E -0 4
0 .0C.O
0 . 00 . 0
1611
5 . 7791:-04 5 .7 7 9 E - 0 4
5 .7 7 9 E - 0 4 5 . 7 7 9 E -0 4
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
5 . 7 7 9 E - 6 4 5 . 7 7 9 E-0 4
b .o0 .0
0 . 60 . 0
1213
5 .7 7 9 E -0 4 5 . 7 7 9 E - 0 4
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
5 .7 7 9 F - 0 45 . 7 7 9 E - 0 4
5 .7 7 9 E - 0 45 .7 7 9 E - 0 4
0 .00 .0
0 . 00 . 0
1415
5 . 7 7 9 ^ - 0 45 .7 7 9 6 -0 4
5 . W 9 E - 0 4 5 .7 7 9 B - 0 4
5 . 7 7 9 ^ - 0 4 5 . 7 7 9 6 - 0 4
5 .Y 7 9 E -0 4 5 . 7 7 9 E -0 4
0 .00 . 0
0 . 00 . 0 •
l i17
li .7 7 9 t ! -o 45 .7 7 9 E - 0 4
5 . ^ 9 E - 0 45 .7 7 9 E - 0 4
S . i7 ^ £ - o45 . 7 7 9 E - C 4
5 . V 7 9 E -6 4 5 . 7 7 9 E - 0 4
6 .00 .0
u . 60 . 0
1819
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 . 00 . 0
0 .00 .0
0 . 00 . 0
2021
f*.00 . 0
0 . 00 . 0
0 . 00 . 0
C .O0 . 0
0 .00 .0
0 . 00 . 0
4 F23
1.5 6 fcF -0 41 .5 8 5 E - 0 4
l , 5 8 5 E - 0 41 . 5 8 5 E - 0 4
1 .5 8 5 C -0 41 .5 8 5 E - 0 4
1 .5 8 5 E - 0 4 1 . 5 8 5 E -0 4
0 .00 . 0
0 . 00 . 0
2425
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 .1 3 9 E - 0 45 .1 3 9 E -U 4
5 .1 3 9 E - 0 45 .1 3 9 F - 0 4
5 .1 3 9 E - 0 4 5 . 1 3 9 F -0 4
Q.O0 .0
0 . 00 . 0
2627
5 . 1 39E— 04 5 . 1 3 9 F -0 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
5 . I 3 9 E - 0 4 5 . 1 3 9 E -0 4
C.O0 .0
0 . 00 . 0
2d29
S .1 3 9 C -6 45 . 1 3 9 E - 0 4
5 . 1 3 ^ - 0 45 . 1 3 9 E - 0 4
5 .1 3 9 E - 0 45 . 1 3 9 E - 0 4
6 . f 3 9 E -0 4 5 .1 3 9 E - 0 4
0 .0C.O
0 . 00 . 0
3031
5 .1 3 9 E - 0 45 . 1 3 9 E - 0 4
5 . 1 3 9 E-C 4 5 .1 3 9 E - 0 4
5 .1 3 9 F -Q 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E - 0 4
0 .00 .0
0 . 00 . 0
3233
, 5 . 1 3 9 E -0 4 5 .1 3 9 E - C 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 .1 3 9 E - 0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
c .oC.O
0 . 00 . 0
3435
5 . 1 3 9 E -0 4 5 . 1 3 9 F - 0 4
5 .1 3 9 E - 0 45 .1 3 9 E - 0 4
5 .1 5 9 E - 0 4 5 . 1 3 9 F -0 4
5 . 1 3 9 E -0 4 5 . 1 3 9 E -0 4
0 .00 .0
0 . 00 . 0
'
3637
5 .1 3 9 F . -0 45 . 1 3 9 F - 0 4
5 .1 3 9 E - 0 45 . I 3 9 E - 0 4
5 . 1 3 9 E - 0 45 .1 3 9 E - 0 4
5 . 1 3 9 E - 0 4 5 . 13*>E-04
c . o0 .0
0 . 00 . 0
3639
5 .1 3 9 E - 0 46 .4 1 0 F - 0 4
5 .1 3 9 E - 0 46 .4 1 0 E - 0 4
5 .1 3 9 E -0 46 . 4 1 0 E - 0 4
5 .1 3 9 E - 0 46 .4 1 0 E - 0 4
0 .00 .0
0 . 00 . 0
416 .4 1 & P -6 46 .4 1 0 E - 0 4
6 . 4 l 6 E - o 4 6 .4 1 0 E - 0 4
t :% lf f F -0 4 '6 . 4 1 0 E - 0 4
t . 4 1 0 t - 6 46 . 4 1 0 E - 0 4
6 .60 .0
Q .O0 . 0
TOTAL FJKEO SOURCE 1*C00001F 00 N/SEC
[c o r e s t o r a g e d i f f e r e n c e c w o r d s > e q u a t i o n c o n s t a n t s I / o __i n s t j e a D O F_STQRED_________ p.
101
EQUATION CONSTANTS WILL BE STOREO IN CORE
NUM8ER OF-------COLUMNS* ROUS. PLANES. GROUPS. UPSCAT. DOWNSCAT. REGIONS. AND ZONES 39 41 1 1 0 0 2!> 5
MEMORY LUCATIONS RESERVED FOR DATA STORAGE------- 40000MEMORY LOCATIONS USED FOR T H IS PROBLEM-----------------MEMORY LOCATIONS NOT USED--------------------------------------------------
2034019660
ZONE MACROSCOPIC CROSS SECTIONS
ZONE NAME GRP D SiGR SIGA NUSIGF BSG POWER/FLUX1 BLANKET 1 I 2 .09500E 00 0 .0 6 .4 2 5 6 0 E -0 2 0 . 0 0 . 0 0 . 0
2 faLANKgT 2 1 2.0950PE 00 0 .0 6 .4 2 5 6 0 E -0 2 0 . 0 0 . 0 0 . 0
3 BLANKET 3 1 Z .09500E 00 0 . 0 6*42560E— 02 0 . 0 C • o 0 . 0
4 SEED 1 2 .2 0 0 7 9 E 00 0 .0 6 .2 1 5 8 0 E -0 2 0 .0 0 . 0 0 . 0
5 M d b ~ S Y R 1 2 .2 J f t T ? e 'f i i f l " O 4 . 9 5 9 l 0 c - 0 2 0 . 0 0 . 0 0 . 0
SttfY iklNU HATRfX
'IB IJF W 1 1
m ' i ......................... ' .................................... .... _ " ■ ■ ' ........ ■ ■■0*0
2 1 0 . 0
3 I 0 . 0
4 1 0 . 0
5 1 0 . 0
102
2 -0 F IX ED SOURCE PROBLEM ( X . Y - NO F IS S IO N SOURCE, AFTER KAPLAN)39X41X1 GROUP, 1599 P O IN T S -
riaoiuil " ri II> n.«i I."1STREAM OF C I T A T I O N CASES ORNL 72
A F IX ED SOURCE PROBLEM FOLLOWSL IN E RELAXATION W ILL BE DONE Ohi ROWS AND COLUMNS - 1 INNER I T E R A T I O N (S )ITER ATION FLUX CHANGE BETA MU-1 M U -2 MU-3 ORIVE FACTOR BALANCE
1 - 2 . 3 1 4 2 0 6 - 0 2 1.0 0 0 0 0 - 0 . 04628 0 . 0 0 . 0 2.1 3798D 13 0 .0 0 0 0 0 02 2 .8 8 0 3 8 E - P I 1.9 7 6 9 0 -1 2 .1 5 8 5 3 -1 2 . 1 5 8 5 3 0 . 0 2*139130 13 0 .9 9 9 4 6 43 -1.97359E-01 1.9 5 4 8 4 - 0 . 8 8 2 5 4 - 0 . 7 0 6 3 8 0 . 0 2.1 3 9 4 9 0 13 0 .9 9 9 8 2 94 - 1 . 4 6 3 7 6 E - 0 1 1.93423 0 .5 9 5 3 0 0 .95131 0 . 0 2.1 3917D 13 1.0001505 - 1 . 2 4 2 8 I E - 0 1 1.9 1 5 3 6 0 .7 2 4 7 7 0 .8 5 5 1 5 0 . 0 2.1 4 2 6 5 0 13 0 .9 9 8 3 7 86 - 8 . 0 4 5 4 2 E - 0 2 1.89841 0 .5 6 6 9 0 0 ,8 9 6 6 9 0 . 0 2 .14750D 13 0 .9 9 7 7 4 37 6 .4 3 9 6 9 E -0 2 1 .8 8 3 4 4 - 0 , 73602 - 0 , 7 1 4 7 2 0 . 0 2 . 15019D 13 0 .9 9 8 7 4 7B 4 .9 6 4 5 4 E -0 2 1.87041 0 .8 2 0 5 7 0 ,6 6 5 8 7 0 . 0 2 .15218D 13 0 .9 9 9 0 7 59 3 .5 6 9 0 3 E -0 2 1.85921 0 .7 5 4 5 9 0 .7 6 7 C 9 0 . 0 2.15355D 13 0 .9 9 9 3 6 5
io - 2 . 5 & 6 2 7 F - 0 2 1.8 4 9 6 9 - 0 . 75050 - 0 , 7 5 0 2 9 0 . 0 2 , 15459D 13 0 .9 9 9 5 1 711 -1 . 8 8 7 6 7 E - 0 2 1.8 4 1 6 9 0 . 71101 0 .7 0 5 0 4 0 . 0 2 .1 5 5 4 2 0 13 0 .9 9 9 6 1 612 -1 . 2 9 6 7 4 E - 0 2 1.8 3 5 0 0 0 .6 7 3 9 8 0 .7 4 8 0 2 0 . 0 2.1 5603D 13 0 .9 9 9 7 1 713 - 1 . 1 0 2 7 2 E - 0 2 1.8 2 9 4 5 0 .8 3 9 3 5 0 .8 1 6 2 0 0 . 0 2.15&48D 13 0 .9 9 9 7 8 814 - 7 . 76708E-03 1 .8 2 4 8 8 0 .6 9 6 5 9 0 .7 9 2 9 4 0 . 0 2 « 156680 13 0.9 9 9 8 1 415 - 6 . 6 2 1 J 4 E - 0 3 1 .8 2 1 1 2 0 .8 4 5 8 5 0 .8 5 8 0 2 0.0 2i'l5 7 2 5 0 13 0 .9 9 9 6 3 216 5 .2 3 0 9 0 S -0 3 1 .8 l § 0 5 -0 . 7 8 4 7 9 - 0 . 7 6 4 1 5 0 , 8 2.1 5 7 5 6 0 13 0 .9 9 9 6 5 417 4 .6 8 9 2 2 E - 0 3 1.8 1 5 5 4 0 .90113 0 .8 3 3 4 1 0 , 0 2.1 5786D 13 0 .9 9 9 8 6 418 3 . ^ 1 l 9 f t - 0 3 1,8 1 3 5 0 0.B 3816 C . 79138 0 . 0 2 .1 5 8 1 1 0 13 Q . 99968319 3 .2 0 6 2 5 E -0 3 1.81185 0. 82281 0 .7 9 6 7 4 0 . 0 2.15831D 13 ‘0 .9 9 9 9 0 420 2 .6 2 6 4 2 E - 0 3 1 .8 1 0 5 0 0 .8 2 1 7 8 0 .8 3 6 9 0 0 . 0 2.1 5847D 13 0 .9 9 9 9 2 821 2 . 3 0 9 8 0 E-0 3 1.8 0 9 4 2 0 .8 6 1 7 6 0 .8 7 9 5 9 0 . 0 2 .1 5 8 6 1 0 13 0 .9 9 9 9 3 5 .
1 ,8 0 3 5 4 0 . 8 ^ 5 0 0 . 86 7C2 0 . 0 2.15873D 13 0 .9 9 9 9 4 223 1 , 6 1 2 6 6 E -0 3 1.8 0 7 8 3 0 ,8 2 2 4 9 0 .8 4 9 2 3 0 . 0 2 .1 5 8 8 4 0 13 0.9 9 9 9 5 124 1 .3 7 9 9 7 E -0 3 1.8 0 7 2 6 0 , 85709 0 .8 7 2 8 5 0 . 0 2.1 5893D 13 0 .9 9 9 9 5 625 1 .1 5 3 9 5 E -0 3 1,8 0 6 8 0 0 .8 3 7 3 7 0 .8 6 3 3 4 0 . 0 2 .1 5 9 0 1 0 13 0 .9 9 9 9 6 326 9 , 8 5 1 4 6 E -0 4 1.80642 0 .8 5 4 7 0 0 .8 5 3 1 6 0 . 0 2.159090 13 0 .9 9 9 9 6 727 6 . 2 3 0 2 1 E -0 4 1.6 0 6 1 2 0 . 83 625 0 .8 6 0 8 8 0 .0
4 .6 0 B l7 fe -0 3 EXTRAPOLATION WITH 5 .6 0 3 6 2.159490 13 Ot.99997228 - 1 . 94848E—04 1 .0 0 0 0 0 - 0 , 2 3 6 9 4 - 0 . 2 0 0 3 5 0 . 0 2J15949D 13 0 .9 9 9 9 9 929 1 .8 5 0 1 3 E -0 4 1.8 0 5 6 9 - 0 , 9 4 9 3 4 - 0 . 7 1 0 3 1 0 . 0 2.1 5950D 13 0 .9 9 9 9 9 730 1 , 23978E— 04 1.80553 0,6 7 0 2 3 0 ,6 6 2 0 5 0 . 0 2.15950D 13 0 .9 9 9 9 9 B31 9 , 2 5 0 6 4 E-0 5 1.8 0 5 4 0 0.7 4 6 2 5 0 .6 1 6 2 5 0 . 0 2.1 5950D 13 0 ,9 9 9 9 9 8
END OF FIX ED SOURCE CALCULATION - I t e r a t i o n T IN E 0 .0 9 8 MINUTES
LEAKAGE 0 . 0 TOTAL LOSSES l.O OCOOE CO TOTAL PRODUCTIONS 0 . 0 REACTOR PUHER(W ATTS) 0 , 0
"BROSS MEUtRON BALANCE '
IjRP L t t LEAkAGF. TOP ifAKAGE R i f LEAKAGE 60T LEAKAGE FNT LEAKAGE BAK LEAKAGE B**2 LOSSES l / V LOSS XENON LOSS 1 0.0_______(M)_______ 00________________ 00_______0.0______ 0.0_______0.0_______ 00_____
SUM 0 . 0 ______________0^0______________0 ; 0 ______________0*0______________0 . 0 ______________<M>______________0 , 0 _____________ 0^0______________0 , 0
■ffRP ABSofipfIjI n s Ou t - s c a t t ^ SQu r CE i N -S C a t t e r ? o t a l l o s s e s t o V a l g a i n s p r o o / a b s c r p1 l.OOOOOE 00 0 , 0 ______________0 . 0 0 .0 _____________ l.OOOOOE 00 0 .0 __________________________________________________(M>___________
SUM l.OOOOOE 00 0 . 0 0 . 0 0 .0 l.OOOOOE 00 0 .0
AVERAGE FLUXES BY ZC1NF ANn GROUP
103
2 ONE I ~ 8 ( . A « C f r |— — i m —
tOWf »
7WI— 5=5iT6---
tDME r.— NOO>SVft“ X iS W J P o i—
MO■tr-
2 -D f |XFO SOURCE PRQBLFM I X .Y - Nil F IS S IO N SOURCE. A U E R M P L A N I________39X41X1 GROUP* 1599 P O IN TS STREAM OF C H A T ION CASES OHNL 72
CROUP 1 t i u x
I1
3 . 6 7 9 0 -0 22
3 .6 8 9 0 -0 23
3 . 7 1 1 0 -0 24
3 .7 2 9 0 -0 25
3 .7 4 2 0 -0 26
3 . 7 4 9 0 -0 27
1 .7 5 1 0 -0 28
3 . 7 4 7 0 -0 29
3 .7 3 9 0 -0 210
3 . 7 2 6 0 -0 211
3 . 7 0 8 0 -0 223
3.6446-623 .7 0 6 0 -0 2
3 .6 9 8 6 -0 23 .7 1 6 0 -0 2
3 .7 2 0 0 - 0 23 .7 3 8 0 -0 2
3 * 7 3 8 0 -0 2 3 . 756D-02
3 .7 5 0 0 -0 23 .7 6 8 0 -0 2
3 * 7 5 7 0 -0 23 . 7 7 5 0 - 0 2
3 * 7 5 9 0 -0 2 . 3 .7 7 6 0 - 0 2
3* 7*6 0 -0 2 3 .7 7 3 0 -0 2
3* 7 4 7 0 -0 23 .7 6 4 0 -0 2
3 .7 3 4 0 -0 23 . 7 5 0 0 - 0 2
3 .7 1 6 0 -0 2^ .7 3 1 0 -0 2
45
3 .7 3 4 W -0 23 .7 7 2 0 - 0 2
3 . 7 4 4 0 - t t3 .7 8 1 0 -0 2
3 .7 6 5 0 -0 23 .8 0 2 0 -0 2
3 .7 8 3 0 -0 23 * 8 2 0 0 -0 2
3 .7 9 5 0 -0 23 .8 3 1 0 -0 2
3 * 8 0 1 0 -0 23 . 8 3 7 0 - 0 2
3 * 8 0 2 0 -0 23 .8 3 8 0 -0 2
3 * 7 9 8 0 -0 2 3 .8 3 3 0 -0 2
3 * 7 8 9 0 -0 23 * 8 2 2 0 -0 2
3 .7 7 4 0 -0 23 . 8 0 7 0 - 0 2
3 * 7 5 5 0 -0 23 .7 8 7 0 -0 2
67
3 .8 1 9 0 -0 2 3 .8 7 7 0 -0 2
3 .8 2 9 0 - 0 23 .8 8 6 0 -0 2
3 .8 5 0 0 -0 23 .9 0 7 0 -0 2
3* 8 6 6 0 -0 2 3 * 9 2 3 0 -0 2
3 * 8 7 7 0 -0 2 3 . 9 3 4 C -0 2
3 * 8 8 3 0 -0 23 . 9 3 8 0 - 0 2
3 * 8 8 2 0 -0 23 .9 3 7 0 -0 2
3 * 8 7 6 0 -0 23 * 9 3 0 0 -0 2
3 .8 6 S 0 -0 23 * 9 1 8 0 -0 2
3 . 8 4 9 0 -0 2 3 . 9 0 C D -0 2
3 .8 2 7 0 - 0 23 . 8 7 7 0 -0 2
ff -9
3 .9 4 6 0 -0 2 4 .0 2 7 0 - 0 2
3*4546-024 . 9 3 6 0 -0 2
3 .9 * 5 0 -0 24 .0 5 5 0 - 0 2
3 * 9 9 1 0 -0 24 .0 7 1 D -0 2
4 .0 0 1 0 -0 24 .0 8 0 0 -0 2
4 * 0 0 5 0 -0 24 * 0 8 2 0 -0 2
4 * 0 0 2 0 -0 24 . 0 7 9 0 -0 2
3 * 9 9 4 0 -0 24 * 0 7 0 0 -0 2
3 * 9 8 0 0 -0 24 * 0 5 4 0 -0 2
3 * 9 6 1 0 -0 24*0330-02.
3 * 9 3 6 0 -0 2 4 * 0 0 6 0 -0 2
1011
4 . 1 2 0 0 -0 2 4 * 2 2 6 0 -6 2
4 .1 2 9 0 -0 24 . 2 3 5 0 -0 2
4 .1 4 8 0 -0 2 4 . 2 5 4 D - 02
4 * 1 6 3 0 -0 24 .2 6 B D -0 2
4 .1 7 1 0 -0 2 4 .2 7 5 0 -0 2
4* 1 7 2 D -0 2 4 * 2 7 6 0 -0 2
4 * 1 6 8 0 -0 24 * 2 7 0 0 -0 2
4 .1 5 7 0 -0 2 4 . 2 5 7 0 -0 2
4 .1 4 0 0 - 0 24 * 2 3 8 0 -0 2
4 * 1 1 6 0 -0 24 * 2 1 3 0 -0 2
4 * 0 8 7 0 -0 2
12"13
4'. 3 4 7 0 -0 2 4 .4 8 3 0 -0 2
4 . 3 5 5 0 -0 24 .4 9 1 0 -0 2
4 .3 7 4 0 -0 24 .5 0 9 0 - 0 2
4 * 3 8 7 0 -0 24 * 5 2 2 0 -0 2
4 * 3 9 40-024 * 5 2 8 0 -0 2
4 * 3 9 3 0 -0 24 * 5 2 7 0 -0 2
4 * 3 8 6 0 -0 24 .5 1 8 0 -0 2
4 .3 7 2 0 - 0 2 4 .5 0 3 0 - 0 2
4 * 3 5 1 0 -0 24 * 4 7 9 0 -0 2
4 * 3 2 3 0 -0 24 * 4 4 8 0 -0 2
4 * 2 8 7 0 -0 24 * 4 0 9 0 -0 2
i r is
4 . 6 3 5 0 -0 24 .8 0 4 0 -0 2
4 .6 4 3 0 -0 24 .8 1 2 D -0 2
4 .6 6 0 0 -0 24 .8 3 0 D -0 2
4 * 6 7 3 0 -0 2 4 .8 4 2 0 -0 2
4 * 6 7 9 0 -6 2 4 .8 4 8 C — 02
4 * 6 7 7 0 -0 24 .8 4 6 0 —02
4*66110-024 * 8 3 6 0 -0 2
4 .6 5 0 0 -0 24 .8 1 7 0 - 0 2
4* 6 2 5 0 -0 24 * 7 8 9 0 -0 2
4 * 5 9 0 0 -0 24 . 7 5 2 0 - 0 2
4 * 5 4 7 0 -0 24 .7 0 5 0 -0 *
1617
4 .9 9 1 0 -0 25 . 1 9 8 0 -0 2
5 * 0 0 0 0 -0 25 .2 0 6 0 -0 2
■5.0180-025 . 2 2 6 0 -0 2
5 .0 3 1 0 -0 2 5 .2 4 2 0 -0 2
5* 0 3 80-025 * 2 4 90-02
5 .0 3 6 0 - 0 25 .2 4 9 0 - 0 2
5 * 0 2 6 0 -0 25 * 2 3 9 0 -0 2
5 .0 0 5 0 -0 25 . 2 1 8 0 -0 2
4 * 9 7 5 0 -0 25 * 1 8 5 0 -0 2
4 * 9 3 4 0 -0 25 * 1 4 1 0 -0 2
4 * 8 8 2 0 -0 25 * 0 8 4 0 -0 2
1619
5 .? 8 B D -0 25 .5 5 2 0 -0 2
5 * ^9 ? D -0 25 .5 6 2 0 -0 2
5 .4 1 6 D -C 25 . 5 8 1 0 -0 2
5 * 4 3 3 0 -0 25 * 6 0 1 0 -0 2
5 .4 4 3 0 -0 25 .6 1 4 0 -0 2
5 . 4 4 4 D -0 25 .6 1 B D -0 2
5* 4 3 50-025 * 6 1 0 0 -0 2
5 .4 1 4 0 -0 25 .5 8 9 0 -0 2
5 * 3 8 0 0 -0 25 .5 5 3 0 -0 2
5 . 3 3 2 0 -0 25 * 5 0 4 0 -0 2
5 * 2 ) 1 0 -0 2 5 . 4 3 9 C -0 2
2621
5 . 7 2 5 0 -0 25 .9 C 6 0 -0 2
4* 7366-025 .9 2 5 0 -0 2
4*7626-625 .9 5 9 D -0 2
5 * 7 8 7 0 -0 25 .9 9 3 D -0 2
5 .8 0 5 D -0 26* 0 1 8 0 -0 2
5 * tt i2 D -0 26 * 0 2 9 0 -0 2
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2*23
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2425
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2627
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2829
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*631
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3233
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3637
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Jft39
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4641
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78
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I f18
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2122
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2*28
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2930
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3334
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1611
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1213
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1415
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2021
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2627
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fONE MIMBF8 AT EACH MfrSH INTERVAL1 2 3 4 § 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20
1 1 1 1 1 I 1 1 1 1 1 1 1 1 1 1 1 1 1 I I2 1 1 1 1 I 1 1 1 1 1 1 1 1 1 1 1 1 1 1 13 1 1 1 1 I I 1 1 1 1 1 1 1 1 1 1 1 1 \ I _ _4 i i 1 1 i 1 1 i i i — r i 1 1 1 1 1 1 1 15 1 l 1 1 i 1 1 } 1 1 1 1 1 1 I 1 1 1 I 16 1 i 1 1 i 1 1 1 i i i i 1 1 1 1 1 1 1 1r 1 l 1 1 t 1 1 1 i i i i I 1 I 1 1 1 I 18 1 i 1 1 l 1 1 1 1 1 1 1 1 1 1 1 1 1 1 19 1 t 1 1 l 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1
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FISSION SOURCE DlSTRIHUtlON AMD SUN l.OCOOO l.OCOOO
H gStftTPTTTW T f f K » C T nR~gg HgS---------------------- --------------------------------------------------------------
ZN TO i n iUB-ZNS ?1 GMA-SE f T5 CLASS DPL N§X NAME1 1____ 0_______0 O O O O MATERIAL 12 2 0 0 0 0 0 0 MATERIAL 2
■pix'Cft s o u r e r iw u t sEcrniN 026
tbjRte oisrftifiuTian am sum— __ i.ooooe 00 t»ooooD ro _______
TOTAL FIXED SOURCE 8.4000006 01 N/SEC
CORF STORAGE DIFFERENCE tWORDS! EQUATION CONSTANTS I/O 1NSTEA0 OF STORED________ 0
EQUATION CONSTANTS WILL BE STORED IN CORE
NUMBER OF------ COLUMNS, ROWS. PLANES, GROUPSt UPSCAT, DOWNSCAT, REGIONS, AND ZONES 20 20 1 I 0 0 4 2
MEMORY LOCATIONS RESERVED FOR DATA STORAGE------ 40000 - -HEWOBy”LOCATIONS USED I-Off >H1 S WUBLE7F----- ------------E973---------------------------------------------------------------------------------------------------------------------------MEMORY LOCATIONS NOT USED--------------------------------------------- 33027 ______ _____________________________________ ________
ZONE MACROSCOPIC CROSS SECTIONS
ZONE NAME________ GRP D______________ SIGR1 M ATERIAL I 1 2 .2 0 0 2 2 E OQ 0 .0
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LEAKAGE 03 TOTAL tosses ? . 329601: OS TOTAL PRODUCT I Oh s 2.245606 03 REACTOR POMERtWATTSI 2.24S59E 09
CWSS WfUIEOW MLANCg
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ro u e IN PUT BY REGION 1
ZONE NUMBER AT EACH MESH INTERVAL
1 2 3 * 5 6 7 8 9 20 I I 12 13 14 15 16 17 18 i » 2d 21 22
I 1 1 1 1 1 1 X 1 1 I 1 1 1 1 1 1 1 I i 1 i 12 t 1 1 1 I 1 1 1 1 1 1 \ \ I * * \ i I 1 1 13 i 1 I i i 1 1 1 1 I I 1 I 1 1 1 I i i 1 I 1* i 1 1 i i 1 1 1 1 1 1 1 1 1 1 1 I i i I \ 1
F IS S IO N SOURCE D IS T R IB U T IO N AND SUH 0 .9 0 0 0 0 0 .0 9 0 0 0 0 .0 1 0 0 0 0 .0 o • c o • o 0 .0 ........- 1 .0 0 0 0 0
PERTURBATION IN PU T - SEC TIO N 0400 0 0 0 0 0 0 0 0 0 0 0 C. O 0. 0 0 . 0
CORE STORAGE DIFFERENCE 1 WORDSI EQ U ATIO N CONSTANTS I/O IN STEAD OF STORED 1212
EQ UATION fcakStANTS N tLL BE STQREO IN CORE
NUMBER OF------COLUMNS* ItOUS. t>LANES« 3R0UPS, U p S d A f , bdHNStAT, REGIONS, AND ZONES 22 4 1 7 2 4 1 1
MEMORY LfltA 'ltO N S k E ^ h V E D b k f k STORAGE------406q6MEMORY LOCATIONS USED FOR THIS PROBLEM--------------- 63C2MEMORY LO C ATIO N S NOT USED--------------------------------------------------- 33698
2 -0 SEARCH ON ABSORBER. 8ARE SLAB WITH UP SCATTER » AMS BENCHMARK PROBLEM22X4X7 GROUPS, 616 POINTS STREAM OF C I T A T I O N CASES ORNL 72
L IN E RELAXATION WILL BE DONE ON ROWS - 1 INNER I T E R A T I O N S !L I M I T I N G VALUES OF T h £ SEARCH FACTOR FOR ABSGKPTICN AND TCT A‘_ LOSS ARE - l .o O O O O E 00 -2 .7 5 1 2 C E 00ITE R A TIO N FLUX CHANGE SETA MO-1 M U -2 MU-3 K SEARCH FACTOH
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t.nMi 0 .9 2 3 5 3 0 .9 3 i b J 0 .2 3 9 1 9 1 .0 0 0 2 1 8 - 2 . 6 0 2 4 9 0 - 0 124 - I . 2 8 9 5 0 F - 0 2 1 .1 7 8 9 5 0 .9 1 7 8 0 0 .9 4 7 9 1 - 5 . 2 4 8 1 9 1.0 0 0 1 8 9 -2 . 5 9 9 9 5 0 - 0 125 1 . 1 7895 0 .9 1 7 2 5 0 .9 5 2 0 7 1.2 9 9 2 9 1 .0 0 0 1 9 5 - 2 . 5 9 78 7 0-0126 - 1 . 1 1 5 4 1 E - 0 ? 1.1 7 3 9 5 0 .9 1 9 7 2 0 .9 4 9 9 8 0 .7 9 6 8 0
-1 .6 1 8 4 5 E -0 1 EXTRAPOLATION WITH 14.3491 1.001931 -2 . 5 7 0 3 1 0 - 0 12T 1 .9 3 5 9 6 E -C 3 1 .0 0 * 0 0 - 0 . 1 7 1 6 3 - C . 14382 10.61831 1 .0 0 0 0 2 8 - 2 . 5 6 9 9 3 0 - 0 128 2 .6 5 3 J6 E -0 5 I . 1 7 W 5 t . d ^ 6 4 1. loadfi - 0 . 1 8 4 5 8 1*000066 - 2 . ^ 6 9 0 5 0 - 0 129 1 .5 9 3 5 9 E - 0 3 1 .1 7 8 9 5 0. r?772 0 .7 9 3 9 5 - 0 .2 1 4 9 1 1 .0 0 0 0 1 9 -2 .5 6 8 7 * 1 0 -0 130 1 .2 3 5 9 6 E -0 3 1 .1 7 3 9 5 P . 77682 0 .7 2 7 3 0 1 .8 4 9 6 4 0 .9 9 9 9 7 9 - 2 . 5 o 9 0 6 0 - 0 131 1 .0 5 5 7 2 E -0 3 1 .1 7 8 9 5 0.8 5 5 2 2 0 .7 9 4 8 6 0 .2 3 1 0 8 0.999*>76 - 2 . 5 6 9 3 8 0 - 0 132 < J.9 S i0 0 E -0 4 1 .17895 0 .8 4 9 1 3 0 . 8 8 718 - 1 .2 4 3 9 V 0 .9 9 9 9 8 7 - 2 . 5 6 9 5 5 0 - 0 13> 6 .7 5 2 0 1 E -0 4 1 .1 7 8 9 5 0 .7 5 4 6 7 C . 88194 1 .1 6 4 2 3 0.'999999 - 2 . 5 6 9 5 7 0 - 0 1
“ H ' i ; i 7 T 5 5 5 - 0 . 7>*62 7 0 .8 6 2 C 6 0 .3 9 * 0 6 1.0 0 0 0 0 1 — 2 . 5O9560— C l35 3 .7 7 6 5 5 E -0 4 1.1 7 8 9 5 0 .7 5 0 3 8 0 .8 3 4 0 3 - 0 . 0 8 3 4 4 0 .9 9 9 9 9 9 - 2 . 5 6 9 5 7 0 - 0 136 2 . ?942 frE-04 1 .1 7 8 9 5 0 .7 4 0 1 8 0 .8 3 1 6 6 1.53701 0 .9 9 9 9 9 8 - 2 . 5o9 6C 0 -0 137 2*11716 E -0 4 1.17395 0 .7 5 7 8 9 0 .8 5 C 9 3 - 1 . 4 2 7 3 0 0 .9 9 9 9 9 8 -2 . 5 6 9 6 2 0 - 0 138 i.88d ^8 E-o < > 1 .17895 0 .8 9 2 0 8 0 .8 7 5 4 5 1 .7 9 6 2 4 0 .9 9 9 9 9 9 -2 .5 6 9 6 3 D - 0 139 1 .6 8 8 0 0 E - 0 4 1 .1 7 8 9 5 0.89411 0 .8 8 0 3 6 0 .8 5 7 2 3 1 .0 0 0 0 0 0 - 2 . 5 6 9 6 3 0 - 0 140 l * S £ 5 A t t - 6 4 i . l 7 8 ^ S 0.96411 O . s s A i i u . 57927 1.0 0 0 0 0 0 -2 .5 f c 9 & 2 D -0 l41 1 .3 9 2 3 6 F -0 4 1.17895 0. 91 264 0 .8 9 7 74 0 .5 9 7 5 0 1 .0 0 0 0 0 0 - 2 . 5 6 9 6 1 0 - 0 142 1 . 2 6 6 * 9 * - ^ 1 .1 7 8 9 5 0 .9 1 1 0 9 0 .9 0 5 2 7 0 .9 8 6 2 3 1 .0 0 0 0 0 0 - 2 . 5 6 9 6 C0-0143 l*15395E-0<< 1 .1 7 8 9 5 0 .9 0 9 8 9 0 .9 2 0 6 3 1 .0 6 9 3 6 1 .0 0 0 0 0 0 - 2 . 5 b 9 5 9 0 -0 144 I .O 4 4 0 4 E -O 4 T . f ? $ 5 5 ' 0 .9 0 9 2 0 0 .9 * 3 5 4 0 .8 5 2 4 0 1 .0 0 0 0 0 0 - 2 . 5 0 9 5 8 0 - 0 145 9 .6 3 2 1 1 E - 0 5 1 .1 7 8 9 5 0 .9 1 U 2 8 0 .9 5 2 1 0 0 .8 2 8 3 9 1.0 0 0 0 0 1 - 2 . 5 6 9 5 6 0 - 0 1
CONVERGENCE IN D IC A TIO N BV M IN IM IZ IN G THE SUM OF THE SQUARES QF THE R t S l S u E ^ - • R E L A T IV E ABSORPTION 1.00005O 3 K 1 .0000277
FND OF C R I T I C A L I T Y SEARCH - 1 TERATION TIME U .0 4 1 PINUTES
D EN S ITY OF 1/V CROSS SECTION IS - 2 . 56956E-01 • FR AC TIO N ABSORPTIONS I n s e a k c h PARAMETER -0 . 1 9 2 1 8 7
LEAKAGE 4 .4 4 2 5 1 F -0 1 TOTAL LOSSES l.OOOOOE C j TOTAL PRODUCTIONS l.OOOOOE 00 RE AC I UR P O a E H tw A U S l l.OOOOOE Oo
A D JO IN T PROBLEM FOLLOWSI T F R A T ICN FLUX CHANGE BETA MU— I MU-2 MU-3 K
1 6 .2 8 1 3 5 E -P 1 1 .0 0 0 0 0 1.2562 7 - 0 . 2222o 0 . 0 1.000001
? * . 5 7 ? 5 1 F - 0 l 1 .3 4 679 0.9 2 6 2 6 0 .4 3 7 / 1 0 . 0 1.000001? 1 .1 9 1 6 4 F -0 1 1 .2 0 9 7 b 0 .4 5 2 6 3 0 .7 4 4 6 0 0 . 0 1.0 0 0 0 0 14 7 .2 6 1 7 5 F -C ? 1 .1 6 4 4 9 C . 68201 0 .4 2 5 6 3 0 . 0 1.C000G1*\ 4 . 28963?-0.‘* 1 .1 7 9 9 4 0.63361 0 .6 1 0 7 4 0 . 0 I . 000001b - 1 . 1 4 4 0 3 F - 0 2 1.17V12 - 0 . 2 7 8 1 4 - 0 . 6 8 f 15 0 . 0 1.0 0 0 0 0 17 - 1 • 76191E-0'* 1 .1 7 8 9 8 0 .1 5 2 2 5 C . 19704 0 . 0 1.000001< r
- 1 . 6 ? ? 2 j g - 0 5 l . l ? 8 9 5 0 .6 0 7 4 9 0 .0 9 0 2 0 0*0 l.O O O P O l9 2 . 3 2 6 9 T E -0 4 1 .1 7 0 9 5 - 0 . 2 1 6 7 9 - 0 . 4 7 6 7 9 0 . 0 l.Q O O viO l
10 - 8 . » 9 2 3 ? E - 0 5 1 .1 7 8 9 b - 0 . 3 6 0 / 4 -0 .9 3 2 2 4 <?.o 1.0000C1
END OF A D JO IN T CALCULATION - ITE R A T IO N TIME 0 . 0 0 7 MINUTES
CONVFPf.lNCE IN D IC A TIO N *v Th e Sum o f T h e s q u a r e * Ur THE RESI0UES - R E L A T IV E " b SORPTION 1 .0 0 0 0 2 4 8 r 1 .0 0 0 0 2 3 0
6 r 0 « N tu lR d N t s k i & u
6 rp LF1 LEAKAGE TOP LEAKAGE P I T LEAKAGE BOT LEAKAGE FNT LEAKAGE BAK LEAKAbe a* *2 LOSSES l / V LOSS XENON LOSS1 O .C I • 76197E-01 1 .1 2 0 6 4 E -0 2 0 .0 0 . 0 0 . 0 0 . 0 - 3 . 3 1 8 7 6 E - 0 2 0 . 02 0 . 0 5 .6 2 8 1 6 E -0 ? ? .2 8 3 5 2 6 -0 3 0 . 0 0 . 0 0 . 0 0 . 0 - 1 .5 4 5 7 7 5 — 02 0 . 03 0 . 0 3 .2 2 9 6 2 E -0 2 1 .3 1 0 3 4 E -0 3 0 .0 0 . 0 0 . 0 0 . 0 - 1 . 5 5 2 2 7 E - 3 2 0 . 04 0 . 0 2 .0 7 0 3 7 E -6 * 8 . 40000F— 04 0 . 0 0 . 0 0 . 0 0 . 0 -3 . 9 8 0 3 7 6 - 0 2 0 . 05 0 .0 2 .0 3 3 0 0 F -0 2 8 .2 4 * 4 b t - 0 4 0 .0 0 . 0 0 . 0 0 . 0 - 2 . 4 4 2 8 3 E - 02 0 . 06 0 . 0 1 . 323 8 3 E-0 2 5 .3 7 1 1 6 E - 0 4 0 . 0 0 . 0 o . u 0 . 0 - 2 . 9 6 9 3 I E - 02 0 . 07 0 .0 7 . 8 8 1 70E-03 3 . 197 78k- 0 4 0 .0 0 . 0 0 . 0 0 . 0 - 3 . 4 0 9 4 0 E— 02 0 . 0
SUM 0 . 0 4 .2 6 9 2 9 E -0 1 1 . 7 3 2 2 0 6 -0 2 0 .0 0 . 0 0 . 0 0 . 0 • 1 .9 2 1 tf7 c -0 1 0 . 0
GR>* ABSORPTIONS 0 U T -S C 6 T1 ER SOURCE IN -S C A T T E R TOTAL LOSSES TOTAL tiAiNS PROO/A3SCRP1 1.2 9 1 5 fE -0 1 5 . 1 6 626F-01 8 .9 9 9 9 9E-0 1 0 .0 0 .9 9 9 9 9 E -O 1 6 .9 9 9 9 9 6 -0 1 2 .0 0 0 0 0 c 00i 6 . 0 l 5 6 9 6 -0 2 1 .8 0 4 71F-01 8 .9 9 9 9 9 E -0 2 1 .9 3 7 3 5 E — 01 2 . 8 3 7 3 5 E -0 1 2 .83735& -O X 5 .0 0 0 0 0 E -0 13 6 .0 4 0 9 9 F -0 2 1 .2 0 8 2 0 6 -0 1 9 .9 9 9 9 9 E -0 3 1 .8 9 3 1 3 E -0 1 1 .9 9 3 1 3 E -0 1 1 .9 9 3 1 3 E -0 1 6 .6 6 6 6 7 E —O l4 t . £ 4 9 0 4 ^ -0 ! 9 .2 9 4 2 7 E -0 2 6 . 0 2 .2 9 5 8 7 E - 0 1 2 . 2 9 5 8 7 E -0 1 2 .2 9 t » e 7 E -0 l 4 .0 0 0 0 0 E —015 9 .5 0 6 7 9 E - 0 2 1 . 5 2 1 C9E-01 0 . 0 2 .4 3 9 0 3 E -0 1 2 .4 3 9 0 3 E -0 1 2 .4 3 9 0 3 E— 01 2 .0 0 0 0 0 E 006 1 . 1 555 7 F-0 1 1 . 6 5 0 8 U - 0 1 0 . 0 2 .6 4 7 2 0 E -0 1 2 .6 4 7 2 0 E -0 1 2 .6 4 7 2 0 1 -0 1 1 .7 1 4 2 8 E 007 1 .3 2 6 8 4 E -0 1 1 . 1 7941E-01 *♦0 2 .2 4 7 3 3 E - 0 1 2 .2 4 7 3 3 E —01 2 .2 4 7 3 3 E—01 1.66bO ?E 00
SUH 7 .4 i '93 J E -0 1 1 .34S99E 00 9 . 999 9 9 E-0 1 1 .3 4 5 9 5 E 00 2 .3 4 5 9 9 E 00 2.34*>99i- 00
? —D SEARCH ON ABSORBER. HARE SLAB H U H U P S C A TTE R . >NS BENCHMARK PROBLEM 27X4X7 GROUPS. 616 POINT?; STREAM OF C IT A T IO N CASES ORNL 72
T u r m i7 > ii -k T S u L Y DEl V » -K / J K * O E L M -£ » MHERE S REPRESENTS N A C K f. CROSS S E C TIO N S . LAM 0CA(f>H(* N P H I) * 1 .9 5 5 2 3 2 E -0 2
COMP NAME 1 MftTEPIAL 1
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S IG A ,S tG «t,0 H * * 2 h U «S IG F -1 .2 8 3 3 9 5 E 01 1 .2 9 1 5 7 1 E
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0000
COMP NAME GRP. K ------- SIGSIFROM A L L GRPS. K£ TO G RP. M1 M ATFRIAL 1 1 1 .2813956 01 2 .9 8 8 8 3 9 E 00 2 .0 0 0 9 4 4 E 00 1.:539259E 00 1 •8893*SE 00 1 .6 * 0 3 8 OE 00 1 .4 6 * 9 5 6 6 00
? 1 .3 3 7 4 9 8 E 01 3 .1 1 * 8 3 * 6 00 2 .0 8 5 2 9 * 6 00 1 .6 0 4 1 4 6 E 00 1 .9 6 8 9 9 2 E 00 1.7 0 9 5 3 1 E 00 1 .5 2 6 7 1 2 6 00
4 i . f c U o U e 01 3 .7 5 8 7 8 0 E 0 0 2 .5 X 0 * 1 8 6 0 0 I . ' 935793E 00 2 .3 7 6 0 6 8 E 00 2 .0 6 2 9 6 6E 00 1 .8 4 2 3 5 1 E 00
* 1 .4 1 6 2 6 8 E 01 3 .2 9 8 2 6 6 E 00 2 .2 0 8 1 0 6 E 00 l . i l»98620fc 00 2 .0 84S S 3E 00 1 .8 1 0 2 1 2 E 00 1 .6 1 6 6 2 7 6 00
5 2.6*66761: 01 6 .1 6 3 6 8 4 E 00 4 .1 2 6 4 2 3 E 00 3 . 174332c CO 3 .8 9 6 2 7 6 E 00 3 .3 6 2 8 5 BE 00 3 .0211Q 5E 00
6 2 .6 l? 9 * 3 E Ol 6 .0 ? 6 ? 6 * £ 0 0 * .6 8 1 6 1 9 6 00 3 . 1398666 00 $ • 8 5 3 S TIE 00 3 .3 * 6 1 3 3 E 00 2 .9 8 8 3 0 2 E 00
7 2 .6 * 3 * 8 1 6 01 6 .1 6 8 1 U E 0 0 * .1 2 9 3 7 6 6 00 3 . 176613E 00 3 •89907*E 00 3 .3 8 5 2 8 8 6 00 3 .0 2 9 2 7 4 E 00
END OF CASE - TOTAL CPU TIM E WAS 0 .0 9 M INUTES TO TAL CLOCK TIM E MAS 0 .7 9 M INUTES
♦••••••••THIS JOS MAS RUN ON 0 3 -1 1 -7 2 ON THE IBM 360/91*********
2 -0 FAST PEACTOR DIM ENSION SEARCH____________________________________________________27X18X1 wROUP, 2430 P O IN TS STHEAH OF C IT A T IO N CASES ORNL 72
MICROSCOPIC C R O iS -S E C T lO N UPDATING FOLLOWS
*******c o n T r o l o p t I o n 1 4 8*<***«>*#
NEW CROSS S EC TIO N TAPE 8 MADE
Mi c r o s c o p k c r o s s -S E C T Itik u p d a t i n g F 3 L L 6 h 5
••••♦••c o n tr o l ' o *»¥!6h i S <»••*••**
TBE T ! TLE5"0E THE CM 5S SECTlgk SET S PftESENTtY OH 'T Hm i f A T I d i i CROSS S EC TIO N LIBRARY TAPI- A R E -_____________________________________________
1 WHOGENECUS &E5IGN 2 HEACTOR--------------------------------------------TV P g .N U C S ,G R P S .O W S .U P S .X 1 15 5 4 0 0
CENERAL CONTROL IN PU T - S EC TIO N 001
0 0 0 0 0 0 0 0 0 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 J 0 0 1 O O O O O O O O O O O O O I O O O C O
75 100 10 2 3 0 0 0 0 0 0 0 0 0 0 0 0 0 12 fr 12 6 12 241 .5 0 0 0 0 0 E 00 5 .0 0 0 0 0 Q E -0 1 9 .9 9 9 9 9 9 E 0 9 9 .9 9 S 9 9 9 E 23 57o I.OOOOOUE 00 ^
kEiiTfcAN t l - J t PfcflbLEM OESCftlATIO^ - SECTION 6fiS-------------------------------------------------------------------------------------------------------------------
9 3 5 5 I 0 5 5 9 S I 9 5 I 9 9 9 5 5 o o 0 0 o4 .9 9 9 9 9 9 E -0 5 1 . OOOOOOE- 0 5 9 .9 9 9 9 9 9 E -0 5 9 .9 9 9 S 9 9 E -0 5 9 .9 9 9 9 9 9 E -0 5 0 .0979-------------------------979----------------------- ' E SW W M M l . W W 8 F TO '" Sr M a W « - f l l 7 .6 --------------------------------------- ---------
T1PVtTOP»BT<»H~T»ftOnW «FAONT»6ACk ftOUkOAftV Cfihflltm n WS-------------------------------------------------------------- -0 .0 _______________ 4 .6 9 2 0 0 0 E -0 1 4 .& 9 2 0 0 0 E -C 1 0 .0 _______________ 4 .6 9 2 0 0 0 6 -0 1 4 .6 9 2 0 0 0 E -0 1
TWO O IH EN SIO N AL C Y LIN D R IC A L GEOMETRY IR ,* > W IDTH 1 .S 3 8 9 B 9 E 02 H EIG H T 9 .9 0 5 9 9 7 E 01
REGION S P E C IF IC A T IO N S -PT5 'KFGION UlbTH------------------------------------------------------------- ------------------------------- :----------------------------------------*---------------------------------------------------------------------------------------------
_____ A 1 .8 4 8 1 9 9 E 01 7 4 . OOOOOOE OX 3 1 .5 0 0 0 0 0 E 01 5 3 .0 4 2 9 9 9 E 01 5 3 .4 7 4 A 9 9 E 01 3 1.& 2400QE O I
PTS REGION H EIGHT3 1 .5 2 4 0 0 0 E 01 6 3 .8 0 9 9 9 9 E 01 9 4 .5 7 1 9 V 9 E 01 ' “
X -D 1 K . P n iN I S 2 f r - U I K . P U JN iS 18
DISTANCES TO MESH INTERVAL 1 NT Eft FACES
J H I S T . 2 9 .2 4 1 * 1 3 .0 6 9 4 1 6 .0 0 6 5 1 8 .4 8 2 __ 6 2 1 .9 5 1 ? 3 4 .9 4 5 e 4 0 .7 5 5 4 5 .1 1 4 10 5 0 .4 0 4
11 5 4 .5 9 3 20 1 0 3 .9 1 2
1221
5 8 .4 6 21 1 1 .7 2 9
1322
6 3 .8 7 51 1 9 .0 3 4
14 6 8 .8 4 6 23 1 2 5 .9 1 6
1524
7 3 .4 8 21 3 2 .4 4 1 .
1625
8 0 .4 9 41 3 8 .6 5 9
17 8 6 .9 4 2 26_ 1 4 3 .9 1 8
19 9 2 .9 4 3 27 1 4 8 .9 9 2
1928
9 8 .5 0 0J . 5 3 .8 9 9
I O I S T .2 5 .0 8 0
11 5 9 .4 2 03
121 0 . ISO 6 3 .5 0 0
413
15.2406e.580
514
21.59073.660
61*
27.9407 8 .7 4 0
7ft*
34*29(183.820
8I ?
40.64088.900
919
4 6 .4 9 093.980
1019
53*34099.060
OfSTANCCS TO FLUX POINTS
J d I S T .1 6 .5 3 4
10 5 2 .5 4 02
1111.3185 6 .5 7 1
312
14.61161.238
413
17.2886 6 .4 0 7
514
23.69671.202
6 3 1 .6 4 37 7 .0 6 8
7 37.9618 3 .7 8 0
817
4 3 .3 6 98 9 .9 9 2
9Itf
4 8 .1 7 39 5 .8 0 3
19 1 0 1 . 2 « l 20- 1 07 .8 9 1 21 1 1 5 .4 3 9 22 122.523 23 1 2 9 .2 2 0 24 1 3 5 .5 6 6 25 1 4 1 .3 1 3 26 1 4 6 .4 7 7 27 1 5 1 .4 6 5
I o i s t . 1 2 .5 4 0 2 7 .6 2 0 3 12.700 4 18.415 5 24.765 6 31.115 7 37.465 V 43.415 V 50.165
10 5 5 .8 8 0 11 6 0 .9 6 0 12 6 6 .0 4 0 13 7 1 .1 2 0 14 7 6 .2 0 0 15 181.280 16 86.360 17 91.440 18 96.520
« M 6 IwPuT "By rt~gg!ON-----------7 7 7 7 7 73 3 3 5 6 81 1 1 2 5 8
ZONE NUMBER AT EACH MESH INTERVAL
1 2 3 4 5 6 7 8 9 10 n 12 13 14 15 16 17 18 19 20 21 22 23 24 2 5 2 6 21
1 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7c V 7 » 7 7' 1 7 7 ' ? '7 '“ 7 7 "'7 7 7 7 7 7 "7 7 7 7 7 ? 7 > 7 73 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 7 ,7 7 7 7 7 74 3 3 3 3 3 3 3 3 3 3 3 3 i 4 4 4 4 4 6 6 6 6 6 « • •5 3 3 3 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 6 6 6 6 6 8 8 86 3 3 3 3 3 3 3 3 3 3 3 ‘4 3 3 4 4 4 4 4 6 6 6 6 6 8 a 87 3 3 i 3 3 3 3 3 3 3 3 3 3 3 4 4 4 4 4 O 6 6 6 6 8 a 88 3 3 I * 3 4 J J 3 J 5 J 3 3 4 4 4 4 6 6 6 6 i 6 » 89 3 3 3 3 3 3 3 3 3 3 ) 3 3 3 4 4 4 4 4 6 6 6 6 6 8 8 8
10 1 I 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 5 5 5 5 5 S a 811 1 1 1 1 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 5 5 5 5 5 a 4 a12 1 1 t 1 1 i 1 i 1 i i 1 1 1 2 2 2 2 5 5 5 5 5 « • 813 i I 1 1 I i 1 i 1 l i 1 1 1 2 2 2 2 2 5 5 5 5 5 8 a 814 i 1 I i 1 1 1 1 1 1 1 1 1 1 2 2 2 2 2 £ 5 5 i 5 8 a 815 i 1 1 1 1 l 1 i 1 i l 1 1 1 2 2 2 2 It 5 5 5 5 5 8 8 a16 i 1 1 1 1 i 1 i 1 i i :i 1 1 2 2 2 2 2 5 5 5 5 5 8 a 817 i 1 1 1 1 i 1 i 1 l l 1 1 1 2 2 2 2 2 5 5 5 5 5 4 a 818 i 1 1 1 1 l 1 i 1 1 1 1 1 1 2 2 2 2 2 9 i. & 5 5 « a s
D ESC RIPTIO N 0* rT aC W 7 P n 6S"~
2N t o i n SUB-ZNS SIGM A-SET I D l i U u tips. NEK NAME1 I 1 1 0 0 9 0 CORE ZONE 1m i -------?----------------
l A 6 A CORE ZONE 23 3 1 1 0 0 0 0 A X IA L B I M I4 4 1 l 0 0 0 0 A X IA L BLKT 25 5 1 1 0 0 0 0 RADfAL ULKT6 6 1 1 0 0 0 0 CNR RAOL BUT7 8 1 1 0 0 0 0 REFLECTCK
os
t
DESCRIPTION >1F MICROSCOPIC CROSS SECTIONS
SFT NUCr. GRPS UPSC OHSC > T I T L E1
GROUP15 5
UPPER ENERGV0 4 HOt'UGENECUS DESIGN 2 REACTOR HEAN ENERGY 1/V X -S E C T IO N D IS T .F U N C T
12
1.491820E 07 8 .208500E 05
3 .4 9 9 3 8 C E C6 3 .8 7 6 0 7 8 E - 0 4 0 .7 5 3 0 3 7 2 .3 5 1 7 7 0 E OS 1 .1 2 1 9 3 0 E -0 3 0 .2 3 8 0 2 5
34
6 .7 3 7 9 5 0 E 04 9 . U 8 8 1 6 E 03
2 .4 7 d 7 5 0 E 04 3 .O 0 1 6 3 O E -O 3 0 .0 0 6 9 3 8 2.6125909 03 9 . I 4 2 6 6 0 E -C 3 C .O
5SUM
7.485188E 02 2 .7 3 5 9 1 O E -O i 2 .3 7 3 9 7 0 E - 0 2 0 . 01.00 0 0 0 0
INPUT NUCLIDE D 6 N S ITI£ S < N U CLID E NUMBER « OfcNSITVl
ZONES 1 - 1 S U B -M N E INDICATOR 0 AND CONTROL C F TIO N 0! 433
9 .9 6 0 7 0 E - 0 41 .1 3 4 9 0 E -0 2
15 2 .8 9 6 2 0 5 -0 4 31 2 . 9 4 5 9 0 E-0 3
16 2 .7 9 6 9 0 6 -0 5 35 2 .0 7 8 7 0 6 —03
1739
7 .2 1 7 9 0 6 -0 6 5 .1 8 6 5 0 E—04
7432
5 .2 2 4 0 0 6 -0 44 . 3 2 5 5 0 6 -0 4
12V
7 .1 7 9 1 0 6 -0 3 5 . 2 6 2 0 0 6 -0 5
25 8 .2 1 8 6 0 E -0 3 23 1 . 804 8 0 E-0 2
ZONES14
2 - 2 SUB-ZONE 1 .2 6 9 4 0 F -0 3
INDICATOR 0 AND CCNTROL C F TIO N 0 15 3 .9 ? 7 4 0 F -0 4 16 3 .7 9 2 0 0 E -0 5 *7 9.9314C,E—06 74 5 .4 4 4 2 0 6 — 04 l i 6 . 77410E—03
3325
1 .1 3 4 9 0 E -0 28 .2 1 8 6 0 E -0 3
2 .9 4 5 9 0 E -0 3 23 1 . 8 0 4 8 0 E-0 2
35 2 .0 7 8 7 0 E -0 3 39 5 .1 8 6 5 0 6 -0 4 32 4 .3 2 5 5 0 6 -0 4 47 5 .2 6 2 0 0 E - 0 5
1433
lo 2 6 9 4 0 E -0 31 .1 3 4 9 0 E -0 2
15 3 . 9 2 7 4 0 E -0 4 3) 2 . 94590E-O3
l b 3 . 792b06-05 35 2 . 0 7 3 7 0 E -0 3
1739
9 .9 3 1 4 0 6 -0 O 5 . 186 5 0 E-0 4
743?
5 .4 4 4 2 0 6 -0 44 .3 2 5 5 0 6 -0 4
12*7
6 .7 1 4 1 0 6 -0 3 5 .2 6 2 0 0 6 -0 5
2514
8 .2 1 8 6 0 E -C 31 .2 6 9 4 0 E -0 3
23 1 . 8 C 480E-02 15 3 . 9 2 7 4 0 E-0 4 i t , 3 .7 9 2 0 0 E -0 5 17 9 .9 3 1 4 0 E —06 74 5 .4 4 4 2 0 E— 04 I * 6 .7 7 4 1 0 6 -0 3
33?C
1 .1 3 4 9 0 E -0 28 .7 1 8 6 0 E -0 3
31 2 .9 4 & 4 0 E -0 3 .’ 3 1 .8 0 4 8 0 E -0 2
35 2 .0 7 8 7 0 E -0 3 39 5 . 18650E—04 32 4 .3 2 5 5 0 6 -0 4 47 5 . 2 6 2 0 0 6 -0 5
1433
1 .2 6 9 4 0 E -0 3 1»1 3 4 9 0 E -0 2
15 3 . 9 2 7 4 0 E -0 4 31 2 .9 4 5 9 0 E -0 3
16 3 .7 9 2 0 0 E -0 5 35 2 .0 7 8 7 0 E -0 3
1739
9 .9 3 1 4 0 6 -0 6 5 . 186 5 0 E-0 4
7432
5 .4 4 4 2 0 6 -0 44 .3 2 5 5 0 6 -0 4
12*7
6 . 7741C6-03 5 .2 6 2 0 0 E —05
25 8*2186 0 E-03 23 1 . 8 0480E-02
iM fc S14
5 - 3 SltS-^O^E 1*8415 0 F -0 4
INDICATOR 0 AND CCNTROL CFTIO N 0 15 6 .1 S 7 2 0 E -0 6 16 1 .0 0 9 0 0 E -1 5 74 4 .5 1 5 1 0 E - 0 5 *0 2 .1 2 4 8 0 6 -0 5 12 8 . 5 9 6 4 CE—03
3325
1 .1 3 4 9 0 E -0 28 .2 1 8 6 0 E -0 3
31 2 . 9 4 5 9 0 F -0 3 23 1 . 8048 0 E-0 2
35 2 .0 7 8 7 0 6 = 0 3 39 5 .1 8 6 5 0 6 -0 4 32 4 .3 2 5 5 0 6 -0 4 47 5 .2 6 2 0 0 6 -0 5
ZONES 4~ 4 SUB— ZONE INBIC.ATCR 0 AND CCNTROL t F T IC N 01433
1 .4 7 7 7 0 E -0 41 .1 3 4 9 0 E -0 2
15 4 .4 2 4 2 0 E -0 6 31 2 .9 4 5 9 0 E -0 3
16 1 .0 0 C 0 0 E -1 5 35 2 .0 7 8 7 0 6 -0 3
7439
3 .1 8 5 4 0 6 -0 55 .1 ^ 6 5 0 6 -0 4
1032
2 .2 1 2 0 0 6 -0 54 .3 2 5 5 0 6 -0 4
1247
8 .6 4 2 3 0 6 -0 35 .2 6 2 0 0 6 -0 5
25 8 .2 1 8 6 3 E -0 3 23 1 . 8 0400E-02
z 6n £S14
5 - 5 SUB-ZONE 2 .7 4 1 7 0 E -0 4
INDICATOR 0 AND CCrtTKOL C f T lG N 0 15 1 .1 6 8 9 C E -0 5 16 l . O C 0 0 0 6 -1 5 74 8 .6 0 7 7 0 E -0 a 10 2 . 3 3 7 9 0 6 -0 5 12 1 .0 2 3 1 0 6 —02
3325
r . T 6 ^ d t - o 26 .5 4 0 0 0 E -0 3
n 2 .8 7 4 O 0 P -O 3 23 2 . 16400E—02
35 2 . 0 2 8 0 0 6 - 0 ^ 39 5 .0 6 0 0 0 6 -0 4 32 4 .2 2 0 0 0 6 -0 4 47 l.OOOOOE—X5
ZONES 6 - 6 SUB-ZONE INDICATOR 0 AND CCNTROL C F I I O N 01433
1 .1 4 4 8 0 E -0 41 .1 0 7 2 0 E -0 2
15 ' &•1 2 0 0 0 E-0 6 31 2 .8 7 4 0 0 6 -0 3
16 1 .OOOOOE— 15 35 2 .0 2 8 0 0 6 -0 3
7439
1 .U 6 0 0 0 6 -0 5 5 .0 6 0 0 0 6 —04
1032
2 . 8 6 1 9 0 6 -0 5 4 .2 2 0 0 0 6 -0 4
1247
1 .0 4 4 4 0 6 -0 2 l.OOOOOE— 15
25 6 .5 4 0 0 6 E -6 5 iS Z .1 6 4 0 0 E -& 2
ZONES33
7 - 8 SUft-20NE 4 .4 2 8 8 0 E -0 2
IN DICATOR 0 AND CONTROL CFTIO N 0 31 1 .1 4 9 6 0 E -0 * 35 8 .1 1 2 0 0 6 -0 3 3<4 2 .0 2 4 0 0 6 -0 3 32 1 .68800E— 03 47 1 . OOOOOE—15
2$ 4 .^ 6 0 0 0 6 -0 3
s p n rc H -3
INPUT DATA - SEC i1UN 028 3 7 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 C 0
9 . 5 0 0 0 0 E -0 1 l.GOOOflf CO 3 , 0 O.ti 0 .0 0 . 0
HEUT tve CHWftES PftW~OIHE»iBTra*i & M m
121
L E F T TO RIG H T l.OOOOOE OO l.OQCOOl: OO l.UOUOOt: OO l .O O OO O t OO
TOP TO BOTTOM 0 .0 0 .0 5.Q0000E-01
F IS S IL E N UCLID ES------- 10 1* 1 6 ___________F E R T IL E N U C L lD tS ------- 1? 15 'IN TER M ED IA TE NUCLIDES------- WOKE S P E C IF IE DOTHER N UCLIDES------- 17 74STRUCTURAL NUCLIDES------- 33 31 35 39 32SP EC IA L N UCLIDES------- 25 23F IS S IO N PRODUCT N UCLIDES-------NONE S P E C IF IE D
CORE STORAGE DIFFERENCE <WORDS! EQ UATION CONSTANTS I/ O INSTEAD OF STOREO 4549
EQ tJAtlON CONSTANTS WILL BE STORED IN CORE
NUMBER OF-------COLUMNS, ROWS. PLAN ES, GROUPS» U P S C A T. OOWNSCAT. REGIONS* AND iON ES_________27 18 1 S 0 4 10 fl
MEMORY LOCATIO N S RESERVED FOR DATA STORAGE-------- 40000___________________________________________________ ____________________________________MEMORY LOCATIO NS USED FOR T H IS PROBLEM------------------ 18151MEMORY LOCATIO N S NOT USED-------------------------------------------------21649
2 -0 FAST REACTOR DIMENSION SEARCH27X18X5 G R O W , 2490 P O IN TS STREAM Of C l f o t l C N C A iE S ORNL 72
L IN E RELAXATIO N M IL L H i DONE ON ROMS AND COLUMNS - 1 INNER IT E R A T IO N !* )ITCA A TIuN
1FLUX CHANte 1 .9 1 7 9 1 E OC
K « '4£ .0 0 0 0 0
M U-1 . 3 .8 3 5 8 2
M U -2-1 ,9 4 1 2 7
M U-3 C .O ..
K0 .S 3 S M 9
2 2 .7 7 5 3 2 E 0 0 1 .9 0 1 2 6 * .2 2 2 3 7 0 ,0 2 9 3 4 0 ,4 8 2 1 9 0 ,7 6 3 2 6 23 1•246066 Q ! 1 .8 2 0 2 6 1 4 .9 5 0 3 8 . 0 .0 3 0 2 2 0,6 2 & 8 ?_ 0 .8 6 6 1 7 74 2 .6 1 2 8 6 E 00 1 .7 5 8 8 0 2 ,8 2 2 5 5 0 ,0 2 4 6 8 C .5 r 7 7C 0 ,9 3 1 2 7 85 T , 372456 00 1 .7 1 4 8 6 1 0 .1 9 4 0 5 0 .0 9 I J 1 0 ,5 0 5 2 3 0 ,9 7 0 5 2 66 — 2*%l«l5>e 00 1 .6 8 4 7 8 3.3 (1 2 5 8 0*10529 0 ,4 1 0 3 3 0 ,9 8 8 5 9 87 4 .3 5 5 0 9 E 0 0 1 .6 6 4 7 7 5 .8 1 7 2 3 0 ,2 3 2 2 7 0 ,4 5 4 0 1 . 0 .9 9 7 3 7 38 1 .4 6 4 5 5 E 0 0 1 .6 5 1 7 4 1 .8 0 0 8 3 0 ,1 6 4 0 « 0 ,5 3 8 5 2 1 ,0 0 2 3 8 49 -4 .5 5 1 S 1 E -0 1 1 .6 * 3 3 5 -0 .7 6 5 9 3 -0 * 6 6 7 3 3 0 .5 6 0 8 3 1 .0 0 5 3 5 3
10 -2 .4 8 1 2 6 E -0 1 1 .6 3 8 0 0 0 .2 9 7 0 2 0*36961 0 ,5 8 5 5 7 1 ,0 0 7 1 6 711 2 .8 0 8 7 4 E -C 1 -0 .8 5 1 1 1 -1 .6 8 3 7 6 0 ,6 2 2 8 1 1 .0 0 8 3 1 412 8*06293E— 02 0 .3 6 7 6 9 0 ,4 5 6 5 2 0 ,6 * 7 5 3 1 ,0 0 9 0 8 713 -1 • 9 7 7 4 7 6 -0 2 1 .6 3 1 1 0 • 0 .2 6 W 3 -0 .3 3 4 7 5 _ 0 ,7 0 3 8 L 1 .C 2 7 6 1 ?14 -1 .5 / 6 4 4 E -0 2 1 .6 3 0 2 5 0 .7 8 1 4 3 0 ,8 6 9 9 4 f l, 73705 1 ,0 0 9 9 9 7IS 1 .3 2 9 9 0 E -0 2 1 .6 2 9 7 1 -0 .8 3 0 3 1 - - L f 9 i m ? _ ................ .. ......% — fcW H I W i s h t w g - w a t — H W«— fcttffiEB 8:818? EftKt fctBftI S ________ ___________________ u m a * ____0 .W 7 8 7 0 .8 0 7 9 0 0 .< 2 « m 1 .0 1 to i»420 5.5 9 7 1 1 E -0 3
2 .6 4 0 3 7 E -0 21 ,6 28 8 9 0 .83773 0 ,8 1 4 0 7 0 ,82617 EXTRAPOLATION WITH 4*7437 1,011380
i i22
-3 .0 7 1 3 7 E -0 32 .6 5 1 2 1 E -0 4
1 .JO 000 -0 ,5 5 1 8 1 -0 ,7 7 7 3 0 1 ,62884 -0 .0 8 6 0 6 -0 .0 3 8 5 9
4 ,7 72 7 7-0 .0 0 1 1 2
1,0113801,011372
■ i r ^24 1.12534E—04
1,62*82 0 ,6 90 8 $ O . i S t v i 1.62081 0 .6 1 4 7 0 1.18402
• 5 ,4 4 3 9 *1.14560
I ,011369 1,0113*8
2526
9*0599l£—06 5 .9 1 2 7 8 2 -0 5
1.62881 0 ,80518 0 ,4 6 3 0 41 .6 28 8 1 0 ,6 5 2 6 9 1 ,0 47 5 9
1 ,04785 1.01*41
1,011367
27 4 .1 9 6 1 7 6 -0 5 £.22880 0,70972 6 ,1 8 1 (9 0 .998$7 i t O i i M
EM> OF £1SENVALUE CALCULATION - 1TEftAilON TIME 0 .1 Z 0 fU N u lES
t t o iV E & m ICE I N O K t n b N by M i n i n i U n a w i i u » w l h £ lo u d n e s Of- THE MESICUES - K E lA U V C A& SOftPflti* 0 ,9 9 9 9 9 1 7 k l , 9 l t 3 » « 9
2 -0 FAST RfACTQk DIMENSI ON SEARCH27X18X5 GROUPt 2430 P C IN TS STREAM OF C IT A T IO N CASES OMNI t 2
L IN E WELAXATIOM W IlL BE OONE IW ROMS ANQ COLUMNS - 1 l* N F » I f f M T M U f S lIT E R A T IO N FLUX CHANGE BETA N U - l KU--2 * U -3 f.
0 U&OOCQE or i,oo_P*e p.03Qpn«»»gM »»»» o.o
?-D FAST REACTOR DIMENSION SEARCH27X18X5 GROUPt 2430 PO IN TS StKEAM tiF C I T A T I G N CASES ORNL 72
L IN E RELAXATION H I L L BE DONE ON ROWS AND COLUMNS - I INNER I f E f t J T I U N I S IITE R A T IO N
1FLUX CHANGE 4 .6 5 4 5 0 E - 0 2 '
BETA1 .0 0 0 0 0
MU-10.097.09
M U-2- 0 . 0 4 9 3 1
MU-30 . 0
KO .«4 0 * O O
2 1 .01 5 0 7 E 00 1 ,9 0 1 2 6 2 2 .8 2 3 3 5 1 2 .5 2 7 2 9 -0 * 0 0 4 0 2 0 .9 4 8 4 4 53 9 .3 0 4 0 B E -0 1 1 .8 2 ^ 2 6 1 .8 4 7 0 0 1 .7 5 6 6 X 1 .3 8 6 6 2 0 .9 4 3 6 6 04 2 .8 8 8 0 1 E 00 1 .7 5 8 8 0 5 »9V204 0 .1 0 0 8 3 0 .2 3 7 5 5 0 .9 4 X 8 7 75 8 .3 6 7 9 9 E -0 1 1 .7 1 4 8 6 1 .1 2 6 5 5 0 .3 6 3 X 7 0 .2 6 2 9 4 0 .9 4 X 1 3 46 1 .8 3 6 6 7 E -0 1 1 .6 8 4 7 8 0 .4 0 3 2 0 0 .4 4 7 4 1 0 .0 8 9 2 3 0*9408957 8 . 07972 S -0 2 1 .6 6 4 7 8 0 .5 2 0 0 6 0 .3 4 3 1 6 0 .5 4 3 9 6 0*940760B - 4 . 8 7 3 9 5 E - 0 2 1.6 5 1 7 4 - 0 . 6 5 1 9 7 - 0 . 4 3 4 1 8 0 .6 3 3 6 7 0 .9 4 0 6 8 09 - 2 . 7 7 6 8 6 E - 0 2 1 .6 4 3 3 5 0 .5 4 X 9 7 0 .5 3 5 9 7 0 .6 0 2 9 4 0 .9 4 0 0 3 3
IP I .1 6 1 1 9 E - 0 2 1 .6 3 8 0 0 - 0 . 4 0 6 5 6 - 0 . 3 4 7 7 2 0 .3 7 7 1 3 0*94060811 4 .2 5 4 3 4 E -0 3 1.63461 0 .3 7 0 6 3 0 .4 4 0 6 7 - 0 .3 1 0 4 1 0 .9 4 0 5 9 612 - S r i 5 $ 4 6 i - o i 1 .6 3 2 4 6 - 0 . 5 5 6 0 1 - 0 . 4 1 4 2 5 T . a i ' l T T " 0 .9 4 0 5 9 113 - 8 . 6 5 3 4 0 E - 0 4 1.63111 •0.36651 0 .3 7 8 5 4 1 .3 5 6 2 7 0 .9 4 0 5 8 814 3 .7 3 8 4 0 E -0 4 1 .6 3 0 2 4 - 0 . 4 3 1 6 4 - 0 . 6 6 5 5 9 1 .1 X 7 9 2 0.9405e<l15 t '2 .2 5 0 0 8 E -0 4 1.62971 -0 .6 0 2 1 1 - 0 . 4 8 1 1 1 1 .0 7 0 3 0 0 .9 4 0 5 8 716 1 .2 3 0 2 4 E -0 4 1 .6 2 9 3 7 -0 . 5 4 6 6 3 - 0 . 7 1 0 2 9 1 .0 3 5 9 6 0*94038817 - 8 . 4 3 4 0 6 E - 0 5 1 .6 2 9 1 6 - 0 . 6 8 5 6 5 - 0 . 7 5 2 1 9 1 .0 2 0 2 8 0 .9 4 0 3 8 818 4 .4 8 2 2 7 E - 0 5 1 .6 2 9 0 3 - 0 . 5 3 1 4 0 -0 .5 0 4 < i4 l . o i x o f 0 .9 4 0 * 8 8
END OF EIGENVALUE CALCULATION - I T E R A T IO N T IM E 0 .C8 X MINUTES
CONVERGENCE IN D IC A T IO N 8V M IN IM IZ IN G THE SUM OF THE SQUARES OF THE R E S 1CUES - R E L A T IV E ABSORPTION 0 .9 9 9 9 9 3 9 K 0 .9 4 0 5 8 7 3
2-D FAST REACTOR OIHENS1UN StftKlH27X18X5 G'UJUPt 2430 P O IN IS STREAM OF C 1TAT ION CASES ORNL 72
L IN E RELAXATION W ILL BE OONE ON ROWS AND COLUMNS - 1 INNER I T E R A T l U N ( S tIT E R A T IO N FLUX CHANGE BETA MU-1 M U -2 MU-3 K
1 - 4 . 1 3 1 3 8 E - 0 3 1 .0 0 0 0 0 - 0 . 0 0 8 2 6 0 .0 0 3 9 9 0 . 0 0 .9 4 9 6 3 82 - 4 . 9 8 1 8 2 E - 0 2 1 .9 0 1 3 4 1 2 .0 0 8 6 7 8 .4 9 9 9 4 - 0 . 0 0 0 1 0 0 .9 4 9 4 4 03 8 . 1 0 6 1 4 E -0 2 1.8 2 0 4 C - 1 . 5 4 6 0 8 -1 . 7 8 7 C 4 - 3 . 2 4 7 6 9 0 .9 4 9 7 6 54 -4 . 4 3 9 4 9 E - 0 2 1 .7 5 8 9 7 - 0 . 59206 - 0 . 7 6 8 8 1 0 .1 5 6 9 3 0 .9 4 9 8 4 25 - 3 . 6 2 7 0 8 E -0 2 1 .7 1 5 0 5 0 .7 6 0 7 3 0 .6 9 7 4 5 0 .3 2 6 8 2 0 .9 4 9 8 8 06 1 .9 2 5 8 5 E - 0 2 1.6 8 4 9 6 - 0 .5 1 1 7 1 - 0 . 5 8 8 5 8 0 .4 0 5 7 6 0 .9 4 9 9 0 17 - 8 . 3 5 4 1 3 E - 0 3 1 .6 6 4 9 5 - 0 . 4 4 2 1 4 -0 . 7 1 7 8 3 0 .9 0 0 8 4 0 .9 4 9 9 1 68 3.5 5 3 3 9 i= -0 3 1.65191 - 0 . 42179 —0 .3 6 8 0 0 0 .8 6 8 8 3 0 .9 4 9 9 2 69 ‘ lc 505 8 5 E-0 3 1 .6 4 352 0 .4 2 5 2 8 0 .4 6 2 6 7 0 .9 3 8 9 7 0 .9 4 9 9 3 3 ,
10 - 9 . 3 7 4 0 2 E -0 4 1.6 3 8 1 6 - 0 . 6 2 3 4 4 - 0 . 2 6 3 5 5 0 .9 4 7 5 9 0 .9 4 9 9 3 711 - 2 . 1 8 2 7 2 E - 0 4 1.6 3 4 7 6 0 .2 3 2 6 3 0 .7 1 5 4 1 0 .9 6 2 1 1 0 .9 4 9 9 4 112 1 .3 9 2 3 6 E - 0 4 1.63261 - 0 . 6 3 7 7 6 - 0 . 4 1 9 8 9 0 .9 7 1 2 7 0 .9 4 9 9 4 313 - 7 . 7 2 4 7 6 E - 0 5 1 .6 3 1 2 5 - 0 . 5 5 4 8 7 - 0 . 6 6 3 9 7 0 .9 8 5 5 7 0 .9 4 9 9 4 514 4 . 76 83 7 E -0 5 1.6 3 0 4 0 -0 . 6 1 7 2 4 - 0 . 5 9 0 3 1 0 .9 9 0 0 2 0 .9 4 9 9 4 6
END OF EIGENVALUE CALCULATION - IT E R A T IO N T IM E 0 . 0 6 4 MINUTES
CONVERGENCE I N D ^ t A f iON BY M IN IM IZ IN G THE &UM OF tH E SQUARES DF THE RESIDUES - R E L A T IV E ABSORPTION 0 .9 9 9 9 9 2 9 K 0 .9 4 9 9 4 1 7
2-D FAST REACTOR DIMENSION SEARCH27X18X5 GROUP * 2430 P O IN TS STREAM OF C I T A T I O N CASES ORNL 72
L I N E RELAXATION W ILL BE OONE ON ROWS AND COLUMNS - 1 INNER I T E R A T I O N S )IT E R A T IO N FLUX CHANGE
1 6 . 0 0 6 1 5 E -0 5BETA
1 .0 0 0 0 0MU-1
0 .0 0 0 1 2MU-2 MU-3
- 0 . 0 0 0 0 6 0 . 0K
0 .9 5 0 0 0 02 1 .3 0 6 5 3 E -0 43 - 2 . 7 6 6 8 5 E - 0 4
1.901911 .6 2 1 3 4
2 .1 7 4 7 3-2 . 1 1 7 9 8
1 .6 5 3 4 0 0 .0 0 0 0 1 - 1 . 9 3 9 3 0 1 .06652
0 .9 5 0 0 0 00 .9 5 0 0 G 0
4 1 .8 0 2 4 4 E - 0 45 9 .7 2 7 4 8 E - 0 5
1.760111 .7 1 6 2 4
- 0 . 6 5 1 2 6 0 .5 3 9 7 8
- 1 . 2 7 9 4 1 0 .8 7 7 3 4 0 .2 8 4 9 5 0 .8 7 7 1 3
0 .9 5 0 0 0 10 .9 5 0 0 0 2
6 - 2 . 7 2 9 8 9 E - 0 5 1 .6 8 6 1 5 - 0 . 2 8 0 6 6 - 0 . 6 8 5 6 9 0 .9 0 5 6 9 0 .9 5 0 0 0 2
END O F EIGENVALUE CALCULATION - I T E R A T IO N T IM E 0 .0 2 7 MINUTES
CONVERGENCE IN D IC A T IO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESICUES - R E L A T IV E ABSORPTION 0 .9 9 9 9 9 9 0 K 0 .9 5 0 0 0 2 7
I^N ^R R E A C T I V I T Y LOOP SEARCH CONVERGED
ES TIM A TE OF NIDK/DNI SAVED 2 .1 9 7 3 1 7 £ -0 1 F IN A L 2 .3 3 3 1 6 7E-01
TWO DIMENSIONAL C Y L IN D R IC A L GEOMETRY t R . Z ) W IDTH 1 .2 7 0 7 9 7 E 02 HEIGHT 9 .3 1 5 9 8 7 E 01
REGION S P E C IF IC A T IO N S P TS REGION W IDTH
4 1 . 3 7 1 188E 01 7 2 .9 6 7 6 1 6 E 01 3 1 .1 1 2 8 5 7 E 01 5 2 .2 5 7 6 1 4 E 01 5 3 .4 7 4 6 9 9 E 01 3 1 .5 2 4 0 0 0 E 01
" T T 53
REGION HEIGHT 1 .5240Q 0E 01 6 3 .8 0 9 9 9 9 E 01 9 3 .9 8 1 9 8 9 E 01
X - D I R . PO IN TS 27 V - O I R . PO IN TS 18
D ISTAN CES TO MESH IN TERVAL IN TERFACES
J O I S T .2
116 .8 5 6
4 0 .50 23
129 .6 9 6
4 3 .3 8 84
1311.8754 7 .38 9
514
1 3 .7 1 25 1 .0 7 7
615
20.7395 4 .51 7
716
2 5 .92 65 9 .7 1 9
017
30.2366 4 .502
916
34*00468 .95 5
10I**
37.39573.137
20 77.093 z i 85*184 22 9& .$yo 23 9 4 .4 0 9 24 105.807 25 111*640 26 117.140 27 122*211 28 127*080_ j..
2■ B i s r :
5 .0 8 0 3 1 0 .160 4 15.240 5 2 1 .5 9 0 6 2 7 .9 4 0 7 3 4 .290 8 40 .640 9 4 6 .99 0 10 53.340~rr S7*T<K 12 '&?. I M i i 66.613 71.03ft 1* T 5 * U ? * . e a r I t 84.311 18 88.735 19 93 .16 0
d is ta n c e s to f l u x p o in ts
41
D IS T **♦048 2 « . 397 3 10.840 4 1 2 .82 6 5 17.560 6 2 3 .4 7 6 7 28.164 8 3 2 .1 T6 9 3 5 .740
1019
3ft*4fe075.141
l it o
4 i . « 08 1 .2 3 9
1221
"■ * K ¥ 5 JTM .9 5 4
I S22
4 9 .2 6 89 6 .0 5 1
1423
5 2 .82 *102.658
1524
57*177108.865
l o25
6 2 .156114.521
1726
66* 766 119.702
1827
71*077124.069
I O fS T .1
102 » i W
» . S S 2I
l i------T T i J f l "
5 9 .9 7 7a
121 2 .^0 064.401
V13 6 8 .8 2 6
a14
2 4 .76 973.250
615
M . l l *7 7 .67 4 16
37*46482.099
417
43*81586.523
918
50*1659 0 .948
LEAKAGE S .3 3 5 5 K 18 TOTAL LOSSES l t i 0 6 0 5 E 20 TO TA L PRODUCTIONS 1 * 05075k 20 REACTOR POfcERIttATTSJ 2.34500E 09
CROSS NEUTRON BALANCE
6 M L F T LEAKAGE TOP LEAKAGE R I T LEAKAGE SOT LEAKAGE FN T LEAKAGE 6AK LEAkAG t B «* 2 LOSSES L/V LOSS XENON LOSS
0 .0 6.71774E Tf> 1 .1327e>£ 17 0.0 0 .0 0 .0 0 .0 0 .0 0 .0
34
0 .00 .0
3.468836 1.408 9UF
1717
4.95320E1.96216E
1717
0.00.0
0 .00 .0
C.O0 .0
O.C0 .0
0 .00 .0
0 .00 .0
5 0 .0 3.78491E 16 5 *.1270 96 16 0.0 0 .0 0 .0 0 .0 0 .0 0 .0
SUM 0.0 1.435E7F 18 2.0996HE 18 G.O 0 .0 0 .0 0 .0 0 .0 0 .0
GRP ABSOKPTIONS OUT-SCATTER SOURCE IN-SCATTER TOTAL LC55ES TOTAL GAINS PRDD/ABSCRP1 1.25393E 19 7.079126 19 8.35108E 19 0.0 8.35109E 19 8.351088 19 2.42140E 002 2.97429E 19 6.40814E 19 2.63267E 19 6.95842E 19 9.59109E 19 9.59109E 19 1.26277E 003 3.40Q55E 19 3.11104E 19 7.67377E 17 6.51906E 19 6.59581E 19 6.5958QE 19 6.30778E-Q14 2.49293E 19 5.924016 18 0 .0 3.119116 19 3. 11911E 19 3.11911E 19 ....4.90854E-015 5.85266E 18 O.C O.P 5.9417 8E 18 5.94179b lti 5.9417oE 18 5.924656-01
SUM 1.07070E 20 1.71903E 20 1.106U5E 20 1.71908E 20 2.82513E 20 2.a2513fc 20
PCINT DAMAGE RATE 101SP LACEMf NT/CC-SEC) FOR NUCLJCE 33
1 2 3 4 5 6 7 8 9 10 111 6.497E 10 6.46 IE 10 6.**2bE 10 6.391E 10 6 .2 94E 10 6 . 111E 10 5 . 9266 10 5.7386 10 5.547E 10 5.3526 10 5.155E 102 1.5266 11 i . J2<^ n “ r . '3 'n r 11 n i t t b l 11 I.2S76 11 1.250E XX X.2X2E i l 1.1756 11 1.1366 11 1.097E 11 1.0576 113 2.436E 11 2.4236 i i 2.4106 n 2.397E n 2.362E 11 2.295E 11 2.228E 11 2 . 160E 11 2.0916 11 2.020E 11 1.9486 114 1.126E 11 1»12 OF i i 1.114E 11 1.1086 n 1.092E 11 1.062E 11 X.032E 11 1.0016- 11 9.6976 10 9.3786 10 9.0526 105 1.8C0E 11 1.791E u 1.781E 11 1.772E u 1.748E 11 1.701E 11 1.6546 11 1.606E 11 1.5586 11 X.509E 11 1.4596 116 2.812E 11 2.798c n 2.765E 11 2.7716 l l 2.733E 11 2.663E 11 2.592E 11 2.522E 11 2.450E 11 2.378E 11 2.3046 117 4.455E 11 4.434E n 4.413E 11 4.392E n 4.334E 11 4.226E 11 4.119E 11 4.C13E 11 3.907E 11 3.80QE 11 3.691E 116 y.26'3?' '11 " 7 :T r 4 r i t '“ T v i m r U " 7 : u ?e n 7.075E 11 6 .904? lx 6 .73 *6 11 6.5716 11 6.4076 11 6.246E l l 6.084E 119 1.2316 12 1.226E 12 I .2206 12 1.214E 12 1.199E 12 1»17 IE 12 1.143E 12 1.116E 12 1.0896 12 1.0636 12 1.0386 12
10 2.0276 12 2.0176 12 2.008E 12 1.999E 12 1.974E 12 1.927E 12 1.882E 12 1.83 76 12 1.794E 12 I . 7526 12 1.7126 1211 2.555E 12 2.543E 12 2.532E 12 2.520E 12 2.489E 12 2.430E 12 2.373E 12 2.3186 12 2.264E 12 2.2126 12 2.1636 1212 2.9976 12 Z.933E 12 2.970E 12 2.9566 12 2.919E 12 2.8516 12 2.785E 12 2.7216 12 2.658E 12 2.5996 12 2.5426 1213 3.3696 12 3.353E 12 3.338E 12 3.323E 12 3.282E 12 3.206E 12 3.132E 12 3.060E 12 2.991E 12 2.924E 12 Z.861E 1214 ' '3.S77E 12 3 . bii 66 12 3 . 644fe 12 " 3 :s 2 -s r 12 12 3.5066 12 3.420E 12 3.3426 12 3.2676 12 3.195E 12 3.127E 1215 3.9256 12 3.9076 12 3.8906 12 3.872E 12 3.825E 12 3.737E 12 3 .651E 12 3.5696 12 3.4896 12 3.4126 12 3.3406 1216 4.X12E 12 4.093E 12 4.075E 12 4 . 057E 12 4.007E 12 3.9156 12 3.826E 12 3.740E 12 3.656E 12 3.5766 12 3.5016 1217 4.238E 1? 4.2136 12 4.199E 12 4 . ia iE 12 4.130E 12 4.035E 12 3.943E 12 3.S55E 12 3.7696 12 3.687E 12 3 .6096 1218 4.301E 12 4.28 IE 12 4.2626 12 4.2436 12 4.191E 12 4.095E 12 4.0026 12 3.9126 12 3.825E 12 3.7426 i2 3.6636 12
12 13 14_ _ 1 {, , .. “ TT!— ._T7_
ifi 19 2(5 21 221 4.907E 10 4.602F 10 4.298E 10 3.907E IQ 3.445E 10 3.012E 10 2.609E 10 2.235E 10 1.6976 10 1.165E 10 8.0106 092 1 .006E 11 9.438E 10 8.809E 1C 7.996E 10 7.043E 10 b.156E 10 5.326E 10 4.547E 10 3.4116 10 2.3236 10 1.591E 103 1.856E 11 1.741E 11 1.624E 11 1.469E 11 1.293E 11 1.1306 11 9.770E 10 8.312E 10 6.099E 10 4.109E 10 2.804E 104 8.638E 10 8.113E 10 7.560E 10 6.790E 10 5.975E 10 5.2306 10 4.5276 10 3.8536 10 2.698E 10 1.8016 10 1.2266 105 1.395E ! 1 1.3I4E 11 1.228E 11 1.107E 11 9.762E 10 8.5466 10 7.384E 10 6 .264E 10 4.349E 10 2.8516 10 1.908E io6 2 .2 10 6 11 2.6966 l l 1.9626 i i 1 .7 b1E 11 X.577E 11 X » 3b IE 11 1.190E 11 1.003E 11 6.847E 10 4.36 86 10 2.9526 107 3.5546 11 3.380E 11 3.1936 l l 2.926E 11 2.609E 11 2.288E 11 1.9o2E 11 1.639E 11 1 -088E 11 6.6786 10 4.224E 108 5.883E 11 5.63 46 11 5.370E l l 4.986E 11 4.486E 11 3.942E 11 3.364E 11 2.773E 11 -,/61E 11 1.026E 11 6.2516 109 I.CC8E 12 9. 7226 11 9.370E l l 8.871F 11 8.074E 11 7.118E 11 6.049E 11 4.904E 11 2.864E 11 1.577E n 9.2536 10
10 1.6656 12 1.614E 12 X.572E 12 X .5366 12 1.412E 12 1.249E 12 1.0626 12 8.5146 11 4.3826 11 2.268E 11 1 .303 E 1111 2.106E 12 2.045E 12 1 .998E 12 1.959E 12 1.80SE 12 X.599E 12 1.357E 12 1.CB4E 12 5.488E 11 2.785E 11 1.579E ll12 2.476E 12 2.4086 12 -2 .T 5 4 F 12 2.309E 12 2.X31E 12 X.837E 12 1.6Q0E 12 1.2776 12 6.4496 11 3.243E 11 1.8246 1113 2.788E 12 2.712F 12 2.653E 12 2.603E 12 2.403E 12 2.128E 12 1.8046 12 1.439E 12 7.2676 11 3.641E 11 2.038E ll14 3.048E 12 2.966E 12 2.90X6 12 2.847E 12 2.628E 12 2.327E 12 1.9736 12 1.5736 12 7.9496 11 3.975E 11 2 .2196 1115 3.256E 12 3.1696 12 3.100E 12 3.042E 12 2.803E 12 2.487E 12 2.108E 12 1 .&80E 12 8.4976 11 4.2466 11 2.3676 1116 3.413E 12 3.322E 12 3.2 50E 12 3 . 190E 12 2.944E 12 2.607E 12 2.2106 12 1.7626 12 8.9106 11 4.451E 11 2.4786 1117 3.519E 12 3.42 5E 12 3.351E 12 3.289E 12 3.036E 12 2.688E 12 2.27t>6 12 1.8166 12 9.187E 11 4.588E 11 2.554E 11id 3 .5 7 2 e 12 ''3 “ *7 7 F 12 12 T r s s ’s r 12 3.08*6 12 2 .7 2 9 t 12 2.3136 12 1.S446 12 9.3266 11 4.6576 11 2.5926 11
23 24 .....2 5 " 26 .....27 "■1 5.470E 09 3.631E 09 2.323F 09 1.412E 09
UJCO• 082 1.0846 10 7.161E 09 4.496E 09 2.689E 09 1.41IE 093 1.908E 10 1.253E 10 7.572E 09 4.4056 09 2.276E 09
4 8.346E 09 5.491E 09 1.242E 10 6 . 968E 09 3.539E 095 1.283E 10 8.381E 09 1.902E 10 1.062E 10 5.376E 096 1.882E 10 1.215E 10 2.764E 10 1.544E 10 7.807E 097 2.723E 10 1.732E 10 3.939E 10 2 . 196E 10 1.1086 108 3.927F 10 2.456E 10 5.564E 10 3.081E 10 1.5456 109 5.684E 10 3.49 8E 10 7.802E 10 4.2 50E 10 2.103E 10
10 7.927E 10 4.840E 10 1.027E 11 5.449E 10 2.666c 1011 9.533E 10 5.786E 10 1.219E 11 6.419E 10 3.123E 1012 1.095E 11 6* 615E 10 1.393E 11 7.317E 10 3.553E 1013 1.218E 11 7.33 8E 10 1.546E 11 8.115E 10 3.937E 1014 1.323E 11 7.954E 10 1 .676E 11 8.797E 10 4.267E 1015 1.408E 11 8.45 7E 10 1.782E 11 9.354E 10 4.538E 10lf> 1.473E 11 8.840E 10 1.863E 11 9.779E 10 4.744E 1017 1.517E 11 9.099E 10 1.917E 11 1.007E 11 4.883E 1018 1.539E 11 9.230E 10 1.945E 11 1.02 IE u 4.953E 10
fc)VO
2-D FAST REACTOR DIMfcNSILN SfcAKCH 27X18X5 GROUP, 2430 POINTS STREAM OF CITATION CASES'ORNL 72
SUMMARY TABLE OF NEUTRCN LGSStS, ETC •
ZONE CLASS FISSILE FERTILE INTERMEDIATE OTHER STRUCTURAL SPECIAL UNSPECIFIED Sums CONV. RATIO POWER(MM) F ISS ILE i KGSCORE ZONE 1 0.15551 0.18413 0 .0 0.00963 0.02502 0.00193 0.00233 0.37856 0.99942 1.12736E 03 2.99722E 02CORE ZONE 2 0.12737 0.11590 0 .0 0.00639 0.01574 0.00129 0.00146 0.26815 0.74657 S .0887IE 02 3.82534E 0?AXIAL BLKT 1 0.00924 0. 05880 0 .0 0.00027 0.00857 0.00044 0.00081 0.07814 5.97892 7.65C51E 01 5 .74079E 01AXIAL BLKT i 6^5841'? 0.03712 0 .0 6 .0 M 1 2 0.00540 0.00028 0.00051 0 .0 4 02/ 7.21974 4.24683E 01 4.7448VE 01RADIAL BLKT 0.02013 0.10608 0 .0 0.00077 0.01227 0.00063 -0 .00000 0.13989 4.9134a 1.64290E 02 1.92069E 02CNR RADL BKT 0.00307 0.03309 0 .0 0.00003 0.00408 0.00017 -0 .00000 0.04044 10.38188 2.55202E 01 8.62009E 01REFLECTOR 0.0 0.0 0 .0 0 .0 0.01452 0.00007 0.0 0.01459 0 .0 U.O 0. U '
______ —_____ OTHER LOSSES • BASFC ON START-GF -STEP TOTAL LOSSES 0.03197 _ , _ , _ m _ _L j .w —OVERALL 0.32016 6.55(513 6 .6 ....... 0 .01721 0.08561 0.00482 0.00511 i . 00000 1.47256 2.34502 E 03 1.0o738E 03
NUCLIDE fiENsItlES BY MNE Ato SUB-ZONE(NUCLIDE NUMBEft - DENSITY! AT DEPLETION TIME OTO DAYS
ZONE NUMBER 1— CORE ZONE 1TO <575 12 7 .179106-03 ' 14 9.96070E-04 15 2.89620E-04 16 2.79690E-05 17 7.21790E-0623 1.80480E-02 25 8 .21860E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.07870E-0339 5.1 S&50E-04 57 5 .26200E-05 74 5.2240ife-04
ZONE NUMBER 2--CORE ZONE 210 0 .0 12 6 .77410E-03 14 1.26940E-03 15 3.92740E-04 16 3.79200E-05 17 9.93139E-0623 1.80480E-02 25 8.218&0E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.07870E-0339 5.18650E-04 47 5 . 26200E-05 74 5i44420E-04SUB-ZONE NUMBER 1 ’TO 5T0 : 12 6 .77410E-03 14 1.269406-03 15 3.92740E-04 16 3 . 79200E-05 17 9.93140E-0623 1.80480E-02 25 3.21860E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.J7870E-03
’ 39 5 .1 8650E—04 47 5 .26200E-05 74 5.44420E-04SUB-ZONE NUMBER 2_______________________________________________________________________________________________________________________________10 0 .0 12 6 .77410E-03 14 1.26940E-03 15 3.92740E-04 16 S.79200E-C5 17 9.93140E-0623 1.80480E-02 25 8.21860E-03 31 2.94590E-03 32 4.32550E-U4 33 1.13490E-02 35 2.07870E-0359 5 .l66S0E-04 47 5 ,26200E—o£ 74 5.44420E--04SUB-ZONE NUMBER 3_________________________________________________________________________________________________________ ______________________10 0 ,0 12 6 .7741OE—03 14 1.26940fc-03 15 3.92740E-04 16 3.79200E-05 17 9.9314CE-0623 1.80480E-02 25 8.2186QE-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.07870E-0339 5 .18650E-04 47 5 .26200E-05 74 5.44420E-04SUB-ZONE NUMBER 4
T O OTO 12 6 .7741OF-03 T4 1.26940£-03 T§ 3.92 740E-04 16 3 . 792CCE-05 17 9.93140E-0623 1.. 80480F-02 25 8.21860E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.0787GE-0339 5 .1 8650E—04 47 5.2620CE-05 74 5.44420E-04
ZONE NUMBER 3— AXIAL BLKT 1' 10 2 .1 2480E-05 12 8.59640E-03 14 1.84150E-04 15 6.19720E-06 16 1.00000E-15 17 0 .0
23 1 .80480E-02 25 8.2IB60E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2.0787CE-C3-----------53— 5 ; lfi5'50E-'fl4---------2T7— 5i 245TSDE-155----------74 ' 4.5 I5IffE-=ff5-------------------------------------------------------------------------------------------------------------------------------------------------ZONE NUMBER 4— AXIAL BLKT 2
To 2.21200E-05 12 8 . 64230E-03 f4 I.4?770E -04 15“ 4.42420E-06 16 1.00000E-15 17 0 .023 1.80480E-02 25 8.21B60E-03 31 2.94590E-03 32 4.32550E-04 33 1.13490E-02 35 2*Q7H7QE-0339 5 . 186$0E-04 4? 5726200E-05 74 3.185406-05
ZONE NUMBER 5— RADIAL BLKT115 2 .3 i?90E -d5 T2 1.0231 OE-02i F ! 2. 7417o£-04 T5 1.16BS0E-0& lb 1.00000E-15 17 uTo23 2.16400E-02 25 6 . 54000E-03 31 2.87400E-03 32 4.22QC0E-04 33 1.10720E-02 35 2.02800E-0339 5 . 06000E—04 47 I.OOOOOE-15 75 8.60770E-05
ZONE NUMBER 6— CNR RADL BKT10 2 .86190E—05 12 1.04440E-02 14 1.14480E-04 15 2.12000E-06 16 1.00000E-15 17 O.C23 2.16400E-G2 25 6.54000E-03 31 2.87400E-03 32 4.22000E-04 33 1 .10720E-02 35 2.02800E-03
39 5.06000E-04 47 1.00000E-15 I k 1.06000E-05ZONE NUMBER 7— REFLECTOR ______________ ______________
10 0 . 0 12 ? 3 0 . 0 25
0 .04. 3600OE—03
1431
0 . 01 . 1 496UE-02
1532
0 . 01.6 8 8 C 0 E -0 3
1633
0 . 04 .4 2 8 8 0 E -0 2
1735
0 . 08 . 1 1 200E-03
39 2 .0 2 4 0 0 E -0 3 47 ZONE NUMBER 8— REFLFCTOR
1 . OOCOOE-15 74 0 .0
10 0 . 0 12 23 r . o 25
0. 04 . 3 6 1 C jE -0 3
1431
0 . 01 .1 4 9 6 0 E -0 2
1532
0 . 01.6 8 3 C 0 E—03
1633
0 . 04 .4 2 8 8 0 E -0 2
1735
0 .08.1 1 2 0 0 E—03
39 2 .0 2 4 0 0 E-0 3 47 1 . OOOOOE-15 74 0 . 0
END OF CASE - TOTAL CPU TIME WAS 0 .4 5 MINUTES TCTAL CLOCK TIME HAS 1 .7 4 MINUTES ******:>**************************************************************************************************************************V*************************************************’ ;<*****************************************
* * * * * * * * * THIS JOB WAS RUN ON 03-11-72 ON THE IBM 360/91*********
» » » » » » * » * * C IT A T IO N - REVISION 2 (JULY 1971} - SUPPLEMENT 2 < MARCH 197 2)**********
* * * * * « * * * T H IS JOB HAS RUN ON 03-13-72 ON THE IBM 3 6 0 / 9 1 ** * * * * * * *
REFLECTING BOUNDARY IN THETA-R GEOMETRY, CASE A1 WITH BLACK ABSORBER 24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 <F 0 0 1 0 0 0 0 0 0 1 0 0 0 0 0l O O O l O O O l O O O O O O O O O C O O O O O
100 100 ■'*. 2 3 0 0 0 0 0 0 0 0 0 0 0 0 0 2 6 12 6 12 242 .OOOOOOE 00 9.999996E-02 9.999999E 09 9.999999E 23 0 .0 _______________ l.OCOOOOE 00________________
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 0 8 0 0 0 0 0 I 1 1 0 0 0 ? 0 C 0 0 0 0 09 .999999E—05 1.000000E-05 0 .0 - 3 . OOOOOOE 00
9 .999999E—05 9.999999E-05 9.999998E-03 9.899999E-01
9.999999E-055.000000E-01
0 .00 .0
LEFT,TOP,RIGHT,BOTTOM,FRONT, 1JACK BOUNDARY CONDITIONS ARE0 .0 0 .0 0 .0 4.692000E-01 4.692000E-01 4.6920C0E-01
ROD BND. CONSTANTS FOP ZONE 0 .0 0 .0
24.692000E-01
TWO DIMENSIONAL CIRCULAR GEOMETRY IR , THETA1 WIOTH 3.141591E 00 HEIGHT 6.999998F 01
REGION SPECIFICATIONSPTS
2REGION WIDTH 8 .539808E-02 8 1.400000E 00 4 1 . 707963E-■01 8 I . '4COOOOE 00 2 R.539808E--02
PTS REGION HEIGHT6 3 .OOOOOOE 01 4 5 .OOOOOOE 00 4 l.OOOOOOE 01 6 2. 500000E 01
X—D I P. ai POINTS 24 Y-DIR . POINTS 20
DISTANCES TO MESH INTERVAL INTERFACES
J2
OIST.0.043 3 0.085 4 0.260 5 0.435 6 0.610 7 0.785 R 0.960 9 1. 135 10 1.310
1120
1.485 12 1.528 2.531 21 2.706
1322
1.5712.881
1423
1.6133.056
1524
1.65ft3.099
1625
1.8313.142
17 2.006 18 2.181 19 2.356
I DIST.2
1112.247 3 17.320 35.000 12 37.749
413
21.21340.311
514
24.49542.720
615
27.38645.000
716
3 0 .COO 50.042
817
31.32554.620
918
32.59658.843
1019
33.819 62.783
20 66.489 21 70.000
DISTANCES TO FLUX POINTS
J1
DIST.0.021 2 0.064 3 0.173 4 0..348 5 0.523 6 0.698 7 0.873 8 1.048 9 1.223
10 1.39B 11 1.507 12 1.549 13 1.592 14 1.635 15 1.744 16 1.919 17 2.094 18 2.26919 2.444 20 2.619 21 2.794 22 2.969 23 3.078 24 3.120
I OIST.1 8.660 2 15.000 3 19.365 4 22.913 5 25.981 6 28.723 7 30.670 8 31.967 9 33.213
10 34.413 11 36.401 12 39.051 13 41.533 14 43.875 15 47 .*88 16 52.381 17 56.771 18 60.84519 64.663 20 68.267
ZONE INPUT BY REGION1 I I I 12 1 2 1 21 1 1 1 13 3 3 3 3
ZONE NUMBER AT EACH MESH INTERVAL
1 2 3 4 5 6 It 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 ?4
1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I2 1 1 1 1 1 I 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 13 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 1 1 1 1 I 1 1 1 14 1 1 1 1 I 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 I5 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 16 1 1 1 1 1 1 1 1 1 1 1 1 I 1 I 1 1 1 I 1 1 1 17 2 2 1 1 1 1 1 I 1 1 2 2 2 2 1 1 1 1 1 1 1 1 2 28 2 2 1 1 1 1 1 1 1 1 2 2 2 2 1 1 1 1 1 I 1 1 2 29 2 2 1 1 1 1 1 I 1 1 2 2 2 2 1 1 1 1 1 1 1 1 2 2
10 2 2 1 1 1 1 I 1 1 1 2 2 2 , 2 1 1 1 1 1 1 1 1 2 e.11 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 112 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 1 1 1 1 1 1 1 113 1 1 1 1 1 1 1 1 1 1 1 I 1 1 i 1 1 1 \ 1 1 1 1 114 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 115 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 316 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 317 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 318 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 319 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 320 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3
FISSION SOURCE DISTRIBUTION AND SUM 0.60000 0.40000 0 .0 1.00000
PERTURBATION INPUT - SECTION 040O O O O O U O O O 0 0 0 0. 0 0. 0 0. 0
CORE STORAGE DIFFERENCE (WORDSI EQUATION CONSTANTS I/O INSTEAD OF STORED 2008
EQUATION CONSTANTS HILL BE STOREO IN CORE
NUMBER OF— COLUMNS# ROWS, PLANES, GROUPS, UPSCAT, DOHNSCAT, REGIONS, AND ZONES 24 20 I 3 0 I 20 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE----- 40000MEMORY LOCATIONS USED FOR THIS PROBLEM— --------- 11578MEMORY LOCATIONS NOT USED---------------------- ----------- 28422
REFLECTING BOUNDARY ?N THETA-R GEOMETRY. CASE A1 WITH B U C K ABSORBER24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORNL 72
LINE RELAXATION WILL BE DONF ON ROWS AND COLUMNS - 1 INNER ITERATIONS)ITERATION FLUX CHANGE
1 -8.86503E-01BETA
1.00000HU—I
-1 .77300HU-2
0.65961MU-3
0 .0K
0.5364142 -9.01325E-01 1.91652 0.11539 1.99946 -0.03187 0.5841353 1.304426 00 1.84591 -0.142B1 -2.36564 -0 .82257 0.6082004 2.59260F 00 1.79011 4.58015 0.21023 -1.08916 0.6005985 7 .13799E 00 1.74836 9.89120 0.12530 0.27032 0.598343fc 1.42860E OC 1.71836 1.62874 0.6466? -1.10891 0.6038827 -4.576456-01 1.69744 -0 .77799 -0 .56430 0.20517 0.6063208 3 .88820E-01 1.68315 -0 .46079 -0 .84672 0.73899 0.6076 279 2.073126-01 1.67353 0.74049 0.43092 1.38109 0.608962
10 -9.248266-02 1.66711 -0 .53859 -0 .20370 0.48894 0.60962211 - 4 . 93319E-02 1.66285 0.48409 1.23974 0.68529 0.61039512 2.35424E-02 1.66004 -0 .45368 -0.45612 0.86664 0.61082813 -1.358116-02 1.65819 -0 .59046 -0 .30138 0.71992 0.61113714 -9 .782916-03 1.65698 0.71055 0.78197 0.71682 0.61135515 -7.89481E-03 1.65618 0.79911 0.81868 0.76790 0.61151416 -6 .496256-03 1.65566 0.81635 0.77839 0.73813 0.61163417 - 5 . 36257E-03 1.65532 0.82012 0.80138 0.75136 0.61172418 -4 .387806-03 1.65509 0.81384 0.81267 0.74817 0.61179019 -3.64405E-03 1.65494 0.82685 0.83634 0.72539 0.61183920 -3.07566E-03 1.65485 0.84095 0.84677 O’. 74019 0.61187521 -2.61790E-03 1.65478 0.84855 0.85517 0.74695 0.61190222 -2.24435E-03 1.65474 0.85507 0.87916 0.73914 0.61192123 —I.94P43E—03 1.65472 0.86 264 0.896 84 0.74535 0.61193624 -1.68961E-03 1.65470 0.86905 0.90833 0.74643 0.61194725 -1.480946-03 1.65469 0.87501 0.92017 0.74765 0.61195626 - I . 306306-03 1.65468 0.88077 0.98011 0.75881 0.61196227 -1.15860E-03 1.65467 0.88577 0.99019 0.76695 0.61196628 -1.03277E-03 1.65467 0.89037 0.97277 0.77761 0.61197029 -9.24885E-04 1.65467 0.89461 0.96510 0.79460 0.61197230 -8.31485E-04 1.65467 0.89818 0.95667 0.82086
-1.06272E-02 EXTRAPOLATION WITH 12.7791 0.61199731 6.B4738E-04 1.00000 -0 .82283 -0.44112 9.86619 0.61199232 7 .3 0 5 15E-04 1.65467 1.06758 0.46958 0.04199 0.61198933 3.66211E-04 1.65467 0.50167 0.59016 -2.05833 0.61198734 1.66893E-04 1.65467 0.45590 1.34739 0.14051 0.61198535 1 .34468E-04 1.65467 0.80 585 0.38960 -1 .75475 0.61198336 1 . 16348E-04 1.65467 0.86536 0.82511 1.75687 0.61198237 9.82285E-05 1.65467 0.84436 0.78806 1.36465 0.611981
END OF EIGENVALUE CALCULATION - ITERATION TIME 0.132 MINUTES
'COfWE'R'G'ENCr n iD I CAT ION' BV WTNIMrZING T H F SOM OF THE S0'l3A'ffES- n F " m ' 'R F S T T l U E S - ' RELATIV E ABSORPTION— --------K— 0.6119/H6
LEAKAGE 1.60506E 13 TOTAL 1LOSSES 8.77122E 14 TOTAL" PRODUCTIONS 14 rEACTOTT' POWEr I WATTS) l.ffrOTSE 04
ADJOINT PROBLEM FOLLOWSITERATION FLUX CHANGE BETA HU-1 MU-2 MU--3 K
1 9.09544E 29 1 .OCOOO********** -0 .67721 0 .0 0.6119812 8.67655E 00 1.91652 8.67655 1.08209 0 .0 0.6H 9B 13 1.893026 00 1.84591 2.11120 0.546 27 0 .0 0.6119814 1.83442E 00 1.79011 2.80347 0.35413 0 .0 0.6119815 3.899706 00 1.74836 6.02554 0.14049 0 .0 0.6119816 1 .14842E 00 1.71836 1.44291 0.48830 0 .0 0.6119817 4.420156-01 1.69744 0.82690 0.45825 0.0 0.6119818 2 . 15405E-01 1.68315 0.70273 0.62724 0 .0 0.6119819 - 1 . 28175E-01 1.67353 -0.72321 —0.43d48 0 .0 0.611981
10 - 4 . 48965E-02 1.66711 0.30538 0.31326 0 .0 0.611981' 11 3 . 70522E-02 1.66285 -0 .78823 -0.34332 0 .0 0.611981
12 1 .89962E-02 1.66004 0.53169 0.35062 0 .0 0.611981 . . . ________ „ _
13 8.23021E-03 1.65819 0.44148 0.57318 0 .0 D.6119S114 5.82695E-03 1.65698 0.71382 1.83434 0 .0 0.61198115 4.23527E-03 1.6561o 0.73108 0.65080 0 .0 0.61198116 3 .23200E-03 1.65566 0.76635 0.44671 0 .0 0.61198117 2.46143E-03 1.65532 0.76404 0.47986 0 .0 0.61198118 1.95694E-03 1.65509 0.79700 0.63362 0 .0 0.61198119 1.57452E-03 1.65494 0.80616 6.79897 0.0 0.61198120 1.27220E-03 1.65485 0.80927 Or 82379 0 .0 0.61198121 1.03378E-03 1.65478 0.81363 0.83006 0 .0 0.61198122 8.45909E-04 1.65474 0.81911 0.85505 0 .0 0.61198123 6.97136E—04 1.65472 0.82482 0.86912 0 .0 0.611'*8124 5„79834E-04 1.65470 0.83232 0.88665 0 .0 0.61198125 4 . 85420E-04 1.65469 0.83766 0.90746 0 .0 0.6119B126 4.09126E-04 1.65468 ' 0.84324 0.92378 0 .0 0.61198127 3.47137E-04 1.65467 0.84883 0.92888 0 .0 0.61198128 2.97546E-04 1.65467 0.85744 0.96137 0.0 0.61198129 2 . 56538E-04 1.65467 0.86244 0.97128 0.0 0.61198130 2.23160E-04 1.65467 0.87011 U02806 0 .0 0.611981i i 1.94550E-04 i . t 5 4 6 f 0.871^4 1.060 54 0 .0 fl.6 li$ 8 132 1.71661E-04 1.65<t67 0.88252 0.98208 0 .0 0.61198133 1.51634E-04 1.65467 0.88348 0.96945 0.0 0.61198134 1.35422E-04 1.65467 0.89322 0.95914 0 .0 0.61198135 1.21117E-04 1.65467 0.89449 0.95183 0 .0
1.45512E-03 EXTRAPOLATION WITH 12.0142 0.61198136 -1.28984E-04 1.00000 -1 .06509 -0.31623 0 .0 0.61198137 -2.98023E-05 1.65467 0.23102 0.81484 0 .0 0.6119813B -2.80738E-05 1.65467 0.94197 0.22728 0.0 0.611981
END OF ADJOINT CALCULATION - ITERATION TIME 0.093 MINUTES
CONVERGENCE in d ic a t io n BV MINIMIZING THE SUM OP THE SQUARES Of THE RESIDUES - RELATIVE ABSORPTION 0.9999974 k 0 .&119796
GROSS NEUTRON BALANCE
GRP1
LFT LEAKAGE 0 .0
TOP LEAKAGE 10.0
RIT LEAKAGE 0 .0
BOT LEAKAGE 3.04103E 12
FNT LEAKAGE 0 .0
BAK LEAKAGE 0.0
B**2 LOSSES 2.04180E 13
l/V LOSS 0 .0
XENON LO$S 0 .0
23
0 .00 .0
0 .00 .0
0 .00 .0
5.66160E 12 7.34792E 12
0 .00 .0
O.C0.0
1.24056E 13 3.36573E 12
0 .00 .0
0 .00 .0
SUM 0 .0 0 .0 0 .0 1.60506E 13 0 .0 0.0 3.61893E 13 0 .0 0 .0
GRP1
ABSORPTIONS 1.97548E 12
OUT-SCATTER 5.00839E 14
SOURCE5.26273E 14
IN-SCATTER0 .0
TOTAL LOSSES 5.26273E 14
TOTAL GAINS 5.26273E 14
PROD/ABSORP0 .0
23
3.24226E 14 4.98680E 14
5.09394E 14 0 .0
3 .50849E 0 .0
14 5.00839E 14 5.09394E 14
8.51687E 14 5.09394E 14
8.51687E 14 5.09394E 14
2.56510E-019.09631E-01
SUM 8.24882E 14 1 .0 1023E 15 8.77121E 14 1.01023E 15 1.88735E 15 1.88735E 15
AVERAGE FLUXES BY ZONE AND GROUP
ZONE 1—3•41279E 12 3 .52458E 12 1.33401E 12
ZONE 2—____ 2c. 'T -^E 12 2.85193E 12 0 .0
ZONE . - ______________________________3 . b 3 E 11 5.70770E 11 6.60979E 11
REFLECTING BOUNDARY IN THcTA-R GEOMETRY. CASE fll WITH BLACK ABSORBER24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORNL 72
PERTURBATION RESULTS--- O E L T A -K / ( K*DELTA -S> WHERE S REPRESENTS MACRO. CROSS SECTIONS. LAMBDAfPHI* M PH I) = 1.903895F-03
COMP1
NAME GRP 1
SIGA,SIGR,DB**2 - 1 . 176969E 01
NU*SIGF 2 .000514E 01
01FF. COEF. - 1 . 172748E-02
B**2 -I.973775E 01
2 -1.335031E 01 2.062125E 01 -1 .456433E—02 -1.160043E 013 -7.318512E 00 7 .760094E 00 -1.675026E-02 -2.448773E 00
2 1 -1.239777E-01 2.0 3456BE-01 -2.318673E-04 - i . 2700306-012 —I.304851F-01 2 .1 1 8524E-01 -2.026779E-04 -X.584089E-013 0 .0 0 .0 0 .0 0 .0
3 1 -5.121354E-01 8.040180E-01 -6.088134E-03 -7.000889E—012 -6.685605E-01 1 .169436E 00 -6.063506E-J3 - 6 . 832684E-013 —6 .639817E—01 1.196918E 00 —1.4993 21F—0 3 —4 .383607E—01
COMP NAME GRP. K -----SIGSIFROM ALL Gf.PS. KK TO GRP. KI1 1 1.176969E 01 1.2132R6E 01 4.566282E 00
2 1 .295245E 01 1 .335C3IE 01 5.023176E 003 1 .886134E 01 I.944095E 01 7.318512E 00
2 1 1 .239777E-01 1.290932E-01 0 .02 1.253135F-01 1.30485 IE-01 0 .03 0 .0 0 .0 0 .0
3 I 5 . 121354E-01 7.470840E-01 7.687084F-012 4 .619086E-01 6.685605E-01 6.7S1681E-013 4 .7U 916E -01 6.722189E-01 6.639817E-01
END OF CASE - TOTAL CPU TIME WAS 0. 29 MINUTES TOTAL CLOCK TIME WAS 2 .77 MTNUTFS6 * & * 4 * & * 4 4 * 4 4* * 4444444444444444* 44* 4* 4 * 4 4 4 4 4 4 4 * 4 * *4 ***4 *# **4 *4 *4 4 4 *4 4 4 4 * * 4 4 4 4 **** * * * * f t * * * * * * * * * * * * * * * * * * ** * * * * *4 4 4 *4 4 4* 4* 44* * 4444444444* * 44* * 44444* * * 4 4* 4444444* 4* 4* 444* 44444* * 4444* * * * 4* * 444* 4* 44* 4* * 4* 4* * * * * * * * * * * * * • > *
JOB WAS RUN ON 03-15-72 CTT THf IbM 3 6 0 / 9 1 ** * * * * * * *
PERIODIC BOUNDARY IN THETA-R GEOMETRY, CASF A2 WITH BLACK ABSORBER 24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
o o 0 o o o o o o 5 0 o o o o 6 o o i o 6 o o o1 0 0 0 1 0 0 0 1 0 0 1 1 0 0 0 0 0 0 0 0 0 0 0
ioo io o lb z 3 o o o o o o 5 o o o 0 o 5 5 5 T5 5 T? 24'2 .OOOOOOE 00___9.999996E-02 9.999999E 09 9.999999F 2 0 .0 _______________ 1 .OOOOOOE 00________________
NEUTRON FLUX PROBLFM DESCRIPTION - SECTION 003
0 0 0 0 8 0 0 0 0 0 - 1 f - 1 0 0 0 2 0 0 0 0 0 0 0 9 . 9 9 9 9 9 9 E - 0 5 l . O C O O O O E - 0 5 9 . 9 9 9 9 9 9 F - 0 5 9 . 9 9 9 9 9 9 E - 0 5 9 . 9 9 9 9 9 9 E - 0 5 0 . 00 .0 - 3 . OOOOOOE 00 9.99999BE-03 9.899999E-C1 5.000000E-01 0 .0 ________________ _____
LEFT,TOP,RIGHT,BOTTOM,FRONT,BACK BOUNDARY CONDITIONS ARE______________________________________PERIODIC 0 ,0 PERIODIC 4.692000E-01 4.692000E-01 4.692000E-01
ROD AND. tONSTANtS FOR ZONE 20 .0 0 .0 ______ 4.692000E-01
CORE STORAGE DIFFERENCE ( HORDS1 EQUATION CONSTANTS I/O INSTEAD OF STORED 2008
UJ----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- ----------------------------- -qEQUATION CONSTANTS WILL BE STORED IN CORE____________________________________________________________________________________________________
NUMBER OF---- COLUMNS, ROHS, PLANES, GROUPS, UPSCAT, DOWNSCAT, REGIONS, AND ZONES________ 24 ?0 1 3 0 1 20 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE------ 40000MEMORY L O C A T I O N S U S F P FOR T H I S P ROB LEM---------------------- 1 1 5 7 8MEMORY L O C A J IONS NOT (JSED---------------------------------- 28422_____________________________________________________________________________________
PERIODIC BOUNDARY \)n THfcTA-R GEOMETRY. CASE A2 WITH BLACK ABSORBER24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORN* 72
LINE RELAXATION MILL BE OONE ON ROMS ANO COLUMNS - 1 INNER ITERAT TONt S1ITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 -B.86502E-01 1.00000 -1 .77300 0.65929 0 .0 0 .S3S7772 -9.01205E-01 1.91652 0.11538 2.17925 -0 .02215 0.5821713 1.30327E 00 1.84591 -0 .14287 -2 .33636 -1 .49119 0.6079 304 2.62630E 00 1.79011 4.64145 0.15920 -0 .72729 0.6007295 6.34566E 00 1.74836 8.76186 0.14709 0.11917 0.5982666 6.07<*37E-0l 1.71836 0.70374 0.70391 -3 .91373 0.6d42$B "7 -4 .56884E -0 I 1.69744 -1 .20842 -0 .31442 0.18277 0.6069528 3.91133E—01 1.68315 -0 .46496 - i . 47437 0.75301 0.6084469 2.90319E-01 1.67353 1.03257 0.20823 0.944^9 0.609581
to 1.65334E-01 1.66711 0.73482 0.64370 0.62327 0.6102CI11 5 . 89361E-02 1.66285 0.41540 0.72550 0.9096R 0.610638i i -4 .91940E-02 1.66004 -0 .88389 -0.13171 0.87079 d . b l i o i z ~ ' “ “ '13 -2.97485E-02 L. 65819 0.57497 0.75652 0.74252 C .61130314 -1 .5871 IE-02 1.65698 0.51764 0.75969 0.65706 0 .61 I48615 -9.02164E-03 1.65618 0.55941 0.76965 0.71352 0.61161716 -7.27433E-03 1.65566 0.79905 0.77071 0.78136 0.61171317 -5 .83059E-03 1.65532 0.79570 0.77895 0.75727 0.61178318 - 4 . 59677E-03 1.65509 6.76379 0.79789 0.7^664
-1.74596E-02 EXTRAPOLATION WITH 3.7810 0.61203019 3 . 19481E-03 1.00000 -0 .69182 -0 .91826 3.46818 0 . 612C 1320 1.74809E-03 1.65485 0.54891 0.54462 0.00125 0.61200721 I .15204E—03 1.65478 0.66018 0.43564 -24.90323 0.61200022 6.S4738E-04 1.65474 0.59506 0.50831 0.56496 0.61199523 5.10216E-04 1.65472 0.74564 0.80110 0.5891B 0.611.09124 4.03404E-04 1.65470 0.79106 0.91129 0.49468 0.61198825 3 . 12805E-04 1.65469 0 . 77573 0.87602 0.28946 0.61198626 2.45094E-04 1.65468 0 . 78378 0.89465 -0 .32149 0.61198427 1.93596E-04 1.65467 0.79008 0.87661 4.51145 0.61198328 1 .51634E-04 1.65467 0.78340 0.06332 1.57071 0.61198229 1.20163E-04 1.65467 0 . 7925) 0 .8 5 6 7 5 1.26293 0.61108130 9 . 53674E-05 1.65467 0.79375 0 .8 4 4 5 9 1.14788
4.32017E-04 EXTRAPOLATION H lTH 4 .5 3 0 0 0.61197831 - 1 . 73450E-05 1 .00000 -0 .18189 -0 .2 9 0 1 4 6.1 2 2 3 5 0.61197832 - B . 1 0 6 2 3 E - 0 6 1.65467 0.46735 0.57144 0 .2 1 0 4 6 0 .6 1 1 9 7 933 5.72205E-06 1.65467 -0 .70588 -0 .57813 1.08415 0.61197°
ENOOF EIGENVALUE CALCULATION - ITERATION TIME 0.120 MINUTES
CONVERGENCE INDICATION 8Y MINIMIZING THE SUM CF THE SQUARES OF THE RFSIOUES - RELATIVF ABSORPTION 1.0000010 K 0.6110790
LEAKAGE 1.60522E 13 TOTAL LOSSES 8.77126E 14 TOTAL PRODUCTIONS 5 .3 6 7 8 3 E 14 REACTOR POWERIWATTS) 1 .0101CE 04
GROSS NEUTRON BALANCE
GRP LFT LEAKAGE TOP LEAKAGE RIT LEAKAGE BOT LEAKAGE FNT LFAKAG6 BAK LEAKAGE B**2 LOSSES 1/V LOSS XENON LOSSI -4 .27433b 07 0 .0 4.27433E 07 3.04133E 12 0 .0 O.C 2.0418PE 13 0 .0 0 .02 8.14447E 07 0 .0 -8.14447E 07 5.6622 IE 12 0 .0 0.0 I.24C58E 13 c . o f .O3 6.58052E 07 0 .0 -6.58052E 07 7.34864E 12 0 .0 0 .0 3.36587E 12 0 .0 C.O
SUH 1 . 0 4 5 0 0 8 0 .0 -1.04507E 08 1.60S22E 13 TT.6 0.0 3.618«*«E 13 0 .0 F . 6 ■
IGRP ABSORPTIONS OUT-SCATTER SOURCE IN-SCATTER TOTAL LOSSES TOTAL GAINS1 1.97556E 12 5.00841E 14 5 . 26275E 14 0 .0 5.26275E 14 5.26275E 142 3.24226E 5.09396E 14 3.50850P »4 5.006416 14 8.51690E 14 8.51691E 14
PROO/ABSORP0 . 02.56519E-01
3 4.98682E 14 0 .0 0 .0 5.09397E 14 5.0<>39,!E 14 5.0°3O7E 14 9.09628E—01
SUM 8.248P3E 14 1.01024E 15 8.77125F 14 1.01024E 15 1.88736E 15 1.B8736E 15
average Flu xes by zone and group
ZONE 1 —3.41278E 12 3.52458E 12 1.334C1E 12
ZONE 2— _______________________________2 . 7 37 7 5E 12 2 . 8 5 2 C 5 E 1 2 0 . 0
ZONE 3—3.64924E 11 5.70811E 11 6.61027E 11
ZONE AVERAGE POWER DENSITI ESIWATTS/CC» 1.61598E 00 0 .0 0 .0
THE MAXIMUM POWER DENS1TYIWA+TS/CC> AT ROW I AND COLUMN T§ F3 2.626443E 00
THE AVERAGE POWER DENSITY ALONG ROW I IS 2.625729E 00 AND THE RELATIVE POWER DENSITIESI FRACTION OF AVERAGE) ARE9 .997254E-01 9.997341E-01 9.997744E-01 9.999484E-01 1.000144E 00 l.rC0270E 00 1.000271E 00 1.00014feE 00 9.999524E-019.997802E-01 9.997424E-01 9.997352E-01 9.997355E-01 9.997432E-01 9 . 997817E-01. 9.999539E-01 1.000148E 00 1.000272E 001.000270E 00 1.000143E 00 9.999462E-01 9.997715E-01 9.997323E-01 9.997243E-01________________________________________________________
THE AVERAGE POWER DENSITY DOWN COLUMN 18 IS 1.678942E 00 AND THE RELATIVE POWER DENSITIES ARE_______________________________________1 .564343E 00 1.445086E 00 1.337614E 00 1.238172E 00 1.145384F 00 t . 0 l<8205E 00 <J.940«J31E-01 9.507440E-01 9.085980E-018. 676471E-01 7.997390E-01 7.110897E-01 6.407340E-01 6.201540E-01 0 .0 _______________ OjO______________ CM)_______________ OjO____________0 . 0 0 . 0
ENO OF CASE - TOTAL CPU TIME WAS 0 .14 MINUTES TOTAL CLOCK TIME WAS 0 .6 4 MINUTES '*************************************************************************************************************** * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
* * * * * * * * * THIS JOB WAS RUN ON 03-13-72 ON THE IBM 3 6 0 / 9 1 * * * * * * * * *
PERIODIC BOUNDARY IN THETA-R GEOMETRY. CASE A4 WITH BLACK ABSCRBER24X20X3 GROUP, 1440 POINTS STREAM OF CITATION CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
C 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 1 0 0 0 0 01 0 0 0 1 0 0 0 1 0 0 1 1 0 0 0 0 0 0 0 0 0 0 0
100 100 10 2 3 0 0 0 0 0 c 0 0 0 0 0 0 0 2 6 12 6 12 242 .OOOOOOE 00 9.999996E-02 9 .999999E 09 9. 999999E 23 0 .0 1. 000000F 00
TWO DIMENSIONAL CIRCULAR GEOMETRY (R,THETA) HIDTH 3.141591E 00 HEIGHT 6.999998E 01
REGION SPECIFICATIONS.PTS
4REGION WIDTH 1.707963E-01 8 1 .400000E 00 4 1 . 707963E-01 8 1. 400000E 00
PTS REGION HEIGHT6 3.0000006 01 4 5 .OOOOOOE 00 4 l.OOOOOOE 01 6 2 .'560000E 01
X-OIR. POINTS 24 Y-D IR . POINTS 20
DISTANCES TO iMESH INTERVAL INTERFACES
J2
OIST.0 .043 3 0.085 4 0.128 5 0.171 6 0.346 7 0.521 8 0.696 9 0.871 10 1.046
1120
1.2212.267
1221
1.3962.442
1322
1.5712.617
1423
1.6132.792
1524
1.6562.967
1625
1.6993.142
17 1.742 18 1.917 19 2.092
I OIST.2
1112.24735.000
312
17.32037.749
413
21.21340.311
514
24.49542.720
615
27.38645.000
716
30.00050.042
817
31.32554.620
918
32.59658.843
1019
33.81962.783
20 66.489 21 70.000
DISTANCES TO FLUX POINTS
J1
D IS f.0.021 2 0.064 3 0.107 4 0.149 5 0.258 6 0.433 7 0.608 8 0.783 9 0.958
1019
1.1332.179
1120
1 .308 2.354
1221
1.4832.529
1322
1.5922.704
1423
1.6352.879
1524
1,6783.054
16 1.720 17 1.829 18 2.004
I DIST.1
10d.660
34.415c
1115.0CG36.401
312
19.36539.051
413
22.91341.533
514
25.98143.875
615
28.72347.588 16
3b .6 t052.381
817
" S i :'S<!> 7 ~ 56.771
$18
33.21360.845
19 04.663 20 6 b .267
ZONE INPUT BY REGION1 1 1 12 1 2 11 1 1 I3 3 3 3
ZCINE NUMBER AT EACH MESH INTERVAL
1 2 3 4 5 6 7 8 9 10 U 12 13 14 15 16 17 18 19 20 21 22 23 24
1 i 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 1 1 1 12 l l l l l l l l l l l l l l l l l l l l l l l l
3 1 1 1 1 1 1 1 1 1 1 1 I 1 I 1 1 1 1 1 1 1 1 1 14 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 15 1 1 1 1 1 1 1 I 1 1 1 1 1 1 1 1 1 I 1 1 1 1 1 16 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 1 1 1 1 1 17 2 2 2 2 1 1 1 I 1 1 1 1 2 2 2 2 1 I 1 1 1 1 1 18 2 2 2 2 1 1 1 I 1 1 1 1 2 2 2 2 I 1 1 1 1 1 1 19 2 2 2 2 1 1 1 1 1 1 1 2 2 2 2 I 1 1 1 1 1 1 1
10 2 2 2 2 1 1 I 1 1 1 1 1 2 2 2 2 1 1 1 1 1 1 1 111 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 112 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I 1 1 113 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 I I 1 1 1 1 1 1 114 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 115 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 316 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 317 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 318 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 319 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 320 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3 3
CORE STORAGE DIFFERENCE (WORDS) EQUATION CONSTANTS I/ O INSTEAD OF STORED 2008
EQUATION CONSTANTS WILL BE STORED IN CORE
NUMBER OF-------COLUMNS. ROWS. PLANES, GROUPS, UP SC A T. OOWNSCAT, REGIONS. AND ZONES________ 2 * 2 0 I 3 0 1 1 6 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE-------- 40000MEMORY LOCATIONS USED FOR T H IS PROBLEM------------------- 17566MEMORY LOCATIONS NOT USED.------------------------------------------------- 2843*
H-F=-H
PERIODIC BOUNOARY IN THETA-R GEOMETRY, CASE A4 WITH BLACK ABSCRBER24X20X3 GROUP. 1440 POINTS STREAM OF CITATION CASES ORNL 72
.LINE RELAXATION MILL BE DONE ON ROMS AND COLUMNS - 1 INNFR I TER AT 10N(SIITERATION FLUX CHANGE BFTA MU-1 MU-2 MU-3 K
1 -S.86503E-01 1.00000 -1 .77301 0.65929 0 .0 0.5356492 -9.01219E-01 1.91652 0.11538 1.96036 -0 .02894 0.5832223 1.30207E 00 1.84591 -0 .14272 -2 .40078 -1 .15361 0.6074574 2.59157E 00 1.79011 4.58192 0.19712 -0 .56856 0.599431 '5 4.17443E 00 1.74836 5.78520 0.21934 0.13456 0.5984426 6 .92911E-01 1.71836 0.85890 0.33785 -3 .59371 0.6046717 - 4 . 58327E-01 1.69744 -1 .11978 -0 .28820 0.06764 0.607052a 4 . 11564E-01 1.68315 -0 .48641 -0 .87407 1.83162 0.6083669 2.1675 3E-01 1.67353 0.74341 0.36310 1.22841 0.609468
10 6 . 27975E-02 1.66711 0.35252 0.80564 0.62318 0.61011811 -5.42194E-02 1.66285 -0 .91762 -0 .30230 0.86634 0.61060112 -2 .8892 IE-02 1.66004 0.50398 0.31810 0.8180.8 0.61099813 - 1 . 82989E-02 1.65819 0.61505 0.73832 0.74500 0 .6 H 2 7 514 -1.06639E-02 1.65698 0.57210 0.74980 0.68336 0.61145915 -8.53842E-03 1.6561U 0.79214 0.76321 0.72483 0.61159416 -6 .779976-03 1.65566 0.78727 0.76720 0.7723J 0.61169417 - 5 . 3 l7 l5E -0^ 1.65532 0.77893 0.77452 0.74153
-1 .85948F-02 EXTRAPOLATION WITH 3.4787 0.61201918 3 .5 0 189E-03 1.00000 -0 , 65510 -0 .61876 •3.19403 0.61200219 1 .99"d6E-03 1.65494 0.57308 0.57968 0.00331 0.61199520 1.33133E-03 1.65485 0.66704 0.54263 -8 .38447 0.61198821 7.22085E-O4 1.65478 0.54370 0.68603 0.57268 0.611983 ’22 5.34058E-04 1.65474 0.73932 0.75425 0.54466 0.61197923 4.24385E-04 1.65472 0.79507 0.93151 0.43205 0.61197624 3.2997 IE-04 1.65470 0.77786 0.89088 0.05173 0.61197425 2.58446E-04 1.65469 0.78350 0.87376 -9 .19849 0.61197226 2.05040E-04 1.65468 0.79356 0.85775 1.85867
9 .7 1025E-04 EXTRAPOLATION WITH 4.7358 0.61196527 -8.02875E-05 l.OCOOO -0 .39165 -0 .45710 8.24581 0.61196628 -3.Z9018E-05 1.65467 0.40977 0.35557 0.29224 0.61196629 -2.03848E-05 1.65467 0.61954 0.75001 1.18051 0.611966
END OF EIGENVALUE CALCULATION - ITERATION TIME 0.107 MINUTES
CONVERGENCE INDICATION BY HIN1H171MG THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 1.0000019 K 0.6119671
LEAKAGE 1.60520E 13 TOTAL LOSSES 8.77143E 14 TOTAL PRODUCTIONS 5.36782E 14 REACTOR POMERIHATTSI l.O lO lO E 04
ADJOINT PROBLEM FOLLOWSITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3 K
I 9.09569E 29 I .0 0 0 0 0 * * * * * * * * * * -0 .67843 0 .0 0.6119662 1.02837E 01 1.91652 10.28369 1.18297 0 .0 0.6119663 2.94773E 00 1.84591 3.23438 0.48244 0 .0 0.6119664 1. 80527E 00 1.79011 2.41770 0.23406 0 .0 0.6119665 3.91966E 00 1.74836 6.09089 0.22546 0 .0 0.6119666 7.98493E-01 1.71836 1.00221 0.34777 0.0 0.6119667 2.97988E-01 1.69744 0.67118 0.46375 0 .0 0.6119668 2.08034E-01 1.68315 0.90616 0.25181 0 .0 0.6119669 1. 13163E-01 l.u7353 0 .6571 ’ 0.52072 0 .0 0.611966
10 3.30057E-02 1.66711 0.3246 f 0.36936 0 .0 0.61196611 - 1 . 8S519E-02 1.66295 -0.59C02 -0 .88796 0 .0 0.61196612 1 .U 074E -02 1.66004 rO .57809 -0.60231 0 .0 0.61196613 7 . 72476F-03 1.65819 0.70318 0.54554 0 .0 0.61196614 6 . 83689E-03 1.65698 0.89190 0.43321 0 .0 0 .6 l l9 6 t15 5.25475F-03 1.65618 0.77384 0.48311 0 .0 0.61196616 4.05216E-03 1.65566 0.77520 1.03753 0 .0 0.61196617 3 . 14808E-03 1.65532 0.78004 0.59875 0 .0 0.61196618 2 . 49672E-03 1.65509 0.79559 0.48143 0 .0 0.61196619 1.95694E-03 1.65494 0.78576 0.73556 n.Q 0.611966
2021
1.53351E-031.199725-03
1.65485 0.76516 1.65478 0.78354
0.76572 0 .0 0.76496 0 .0
0.6119660.611966
22 9.365088-04 3.1-8051E-0*
1.65474 0.78154 EXTRAPOLATION WITH
0.76383 0 .0 3.3992 0.611966
2324
-3.12388E-04 4 . 57764E-05
1.00000 -0 .33388 1.65470 -0 .14649
-1-.73337 0 .0 -0 .21146 0 .0
0.6119660.611966 -
2$ -S.64580E-65 1.6542.9 -0 .665^9 -0 .62?43 O.d 0.611966
END OF ADJOINT CALCULATION - ITERATION TIME 0.069 MINUTES
CONVERGENCE INDICATION BY MINIMIZING THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 1.0000057 K 0.6119703
GROSS NEUTRON BALANCE
6rP l f t L eakage1 -1.17789E 12
fdA le a Ka Ge 0 .0
T n n o o & E1.17789E 12
dST3.04130E 12
f n V l e a k Ag£ 0 .0
BAK LEAKAGE 0.0
LOOSES 2.04189E 13
l/ v LrtSs 0 .0
xStodto- LOSS 0 .0
2 -6.07286E 113 -7.12042E 11
0*00 .0
6.07286E 7 . 12042E
1111
5.66215E 12 7.34855E 12
0 .00 .0
0.00 .0
1.24062E3.365846
1312
0 .00 .0
0 .00 .0
SUM -2.49722E 12 0 .0 2.49722E 12 1.60520E 13 0 .0 0.0 3.61909E 13 0 .0 0.0
GRP ABSORPTIONS 1 I.97929E 12
OUT-SCATTER 5.00847E 14
SOURCE 5 . 26285E 14
IN-SCATTER0 .0
TOTAL LOSSES 5.26286E 14
TOTAL GAINS 5.26285E 14
PROO/ABSORP0 .0
2 3.24232E 143 4.98689E 14
5.09404E 14 0 .0
3.5C857E0 .0
14 5.00847E 14 5.09404E 14
8.51704E 14 5.09402E 14
8.51704E 14 5.09404E 14
2.56509E-019.09613E-01
SUM 8.24900E 14 1.01025E 15 8.77142E 14 1.31025E 15 1.88739E 15 1.88739E 15
AVERAGE FLUXES BY ZONE AND GROUP
ZONE 1—3.41282E 12 3. 52463E 12 1. 33401E 12
ZbNt 2—2.7429 IE 12 2. 85633E 12 0 . 0
ZONE 3 ~3.64917E 11 5 . 7080 IE 11 6 . 61016E 11
Z P ME~ AVERAGE TOWER 0EN5 n i 'l : S n W m / C C ) 1.61598E OO 0 .0_____________ 0^0
THE MAXIMUM POWER DENSITY(WATTS/CC) AT ROW 1 . AND COLUMN 8 IS 2.626999E 00
THE AVERAGE POWER DENSITY ALONG ROW 1 IS 2.626125E 00 AND THE RELATIVE POWER DENSITIEStFRACTION OF AVERAGE) ARE9.997330E-01 9.997312E-01 9.997378E-01 1.000196E 00 9.999884E-01 9.997995E-01
9.997519E-019.997509E-01
9 .998057E-01 9.999967E-01 1.000202E 00 9.997385E-01 9.997342E-01 9.997367E-01
1 .000332E 00 9.997628E-01
1.000330E OC 9.99915 7E-01
1.00b093E 00 1.000206E 00 1.000200E 00 1.000078E 00 9 .998961E-01 9.997461E-01
THE AVERAGE 1 .563652E
POWER DENSITY OOWN COLUMN 8 00 1.444663E 00 1.337394£ 00
IS 1.3&S646F1.238099E 00
00 AND tHE RELAtlV f POW*:R D^foSITlgS AftE 1.145412E 00 1.058302E 00 9.942247E-01 9 .508932E-01 9 .087605E-01
8 .678176E-01 7.999176E-01 7 . 112684E-01 0 .0 0 .0
6.409082E-01 6 . 203337E-01 0 .0 0 .0
O•O
C.O
PERIODIC BOUNDARY IN T H E TA -R GEOMETRY* CASE A4 WI T H BLACK ABSCRBER 24X20X3 GROUPt 1440 POINTS STREAM OF C I T A T I O N CASES ORNL 72
PERTURBATION RESULTS-----DELTA-K/C K*DELTA -S I WHERE S REPRESENTS MACRO. CROSS SECTIONS. LAMBDA!PH I * M PH II = 1.923210E-03
COMP1
NAME GRP1
SIGA,SIGR.D&**2 -1.176954E 01
NU*SIGF 2.000543E 01
DIFF. COEF. -I.172626E -02
B**2 -1.9737S0E 01
23
•1.335024E 01 -7.318287E 00
2.062161E 01 7.760093E 00
-1.456099E-02-1.678621E-02
—1 .160937E 01 -2.448698E 00
2 12
-1.243766E-01-1.309730E-01
2.C41908E-012.125265E-01
-2.317438E-04-2.028837E-04
-2.277138^-61 -1 .59001 IE-01
331
0 .0-5.121053E-01
0.08.039941E-01
0 .0-6.087616E-03
0.0-7.000477E-01
23
-6.685296E-01-6.639538E-01
1 .169407E 00 1 .196888E 00
-6.063085E-03-1.499188E-03
—6.832368E-01 -4.383423E-01
COMP NAME GRP. K ----- SIGS(FROM ALL GRPS. KK TO GRP. K>1 1 J.. 176954E 01 1.213273E 01 4 . 566157E 00
2 1.295232E 01 1.335024E 01 5.023049E 003 1* 886115E 01 1.944041E ill 7 .31828*6 66
2 1 1.243768E-01 1.294599E-01 0 .02 1.258296E-01 1.309730E-01 0 .03 0 .0 0 .0 0 .0
3 1 5.121053E-01 7.470433E-01 7.O86673E-012 4.618849E-01 6.685296E-01 6.731362E-013 4 » 711695E-01 6.721905E-01 6.639538E-01
END OF CASE - TOTAL CPU TIME WAS 0 . 22 MINUTES TOTAL CLOCK TIME WAS 1.64 MINUTES* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * ********************************* * * * * * * * * * * * * * * * ** * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * # * * * * * * * * * * * * * * * * * * * * * 9 * » * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * H
■P-
5 JOB »A5~ITON ON ON THE IBM 3S0/91*********
R-Z CASE TO CQMPAPE WITH THFTA-R-7 CASE, WITH BLACK ABSORBER______________13X20X4 GROUP, 1040 POINTS STREAM OF CITATION CASfcS ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 1 0 0 0 0 01 0 0 0 1 0 0 0 0 0 0 1 1 0 0 0 0 0 0 0 0 0 a 0
100 lo o lo l .o r o o o c e r-2
29
3 0 0 ,<?999V9F-05
0 0 9.999999E
009
09.
0 0 999999E
012
00 .0
0 0 01
12 6 .OOOOOOE
1200
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
t> 0 0 r 7 0 0 C O O 1 1 o a 0 0 3 0 0 0 0 0 0 09.999999E—05 1„OOOOOOF 9.999998E-03 - 4 . OOOOOOE
-0500
9.999999F-05 6.30C000E 01
9.999999E-05 1 .OOOOOOE 00
9.999999E-05 1 . OOOOOOE 00
0 .00 .0
LEFT,TOP,RIGHT,BOTTOM,FFUNT,BACK BOUNDARY CONDITIONS ARE0 .0 0 .0 ' 9.999998E-03 9.999998E-03 9.99999BE-03 9.999998E-03
R0T5 "RWL TOTT5TA KiT 5 TfTR — 5---------------------------------------------------1.526000F—02 7.453996E-0Z 1.102300E-01 1.242099E-01
TWn DIMENSIONAL CYLINDRICAL GEOMETRY (R ,Z ) WIDTH 2.99999Bfc 01 HEIGHT 4.599998E 01 H------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------_p-\J1
REGION SPECIFICATIONS PT§ RFGION WIDTH
4 1 .OOOOOOE 01 9 2 .OOOOOOE 01
PTS RFGION HEIGHT9 z .a o o o o d f i&T.......... T 1 . OOOOOOE 01 3 6 .C C 0 0 0 OE O O l .< OOGOOUE 01
X - n iR . POINTS 13 Y-OtM . POINTS 20
DISTANCES TD W 5 H N T e r i/AL IN TERFACES
■ j o r s n2 5 .0 0 0 3 7 .0 7 1 4 3 .6 6 0 5 1 0 .0 0 0 6 1 3 .7 4 4 7 1 6 .6 6 7 8 19 .1 4 9 ' 9 21.344 10 23 .3 3 3
11 ?5.1bt> 12 2 6 .8 7 4 13 2 8 .4 8 0 14 Jo .o o o
" i ■ o i s r . - 2 2 .2 ? 2 3 4 .4 4 4 4 6 .6 6 7 5 8 .£ 8 9 6 11 .1 1 1 7 1 3 .3 3 3 b 1 5 .5 5 6 9 17. 77d 10 2 0 .0 0 0
11 2? .5 o ti20 4 3 .5 0 0
1221
2 3 .0 0 04 6 .0 0 0
—I T " 2if.50U 14 3 0 . C qU 15 iiz .M o 16 3 4 .0 0 6 17 3 6 .0 0 0 18 3 8 .5 0 0 19 4 1 .0 0 0
DISTANCES TO FLUX POINTS
J DIST.1 3.536
10 24.2672
116. 124
26.034 127 .9ri>
27.6894
139.354
29.2505 12.019 6 15.275 7 17.951 8 20.276 9 22.361
I DIST.1 1.111
10 21.2502
11? .333
23. 75 C3
125.556
26.2 504
137.778
28.7505
1410.00031.000
615
12.22233.000
716
14.44435.000
a1 1
1 6 .6 6 737.250
9IB
18.68939.750
19 42.250 20 44.750
ZONE INPUT BY REGION1 1__________________________3 I1 1______________ ;___________________2 2
I ONE NUMBER AT EACH MESH INTERVAL
T I % 4 5 c 7 8 9 10 1 1 1 2 13
1 1 1 I 1 1 1 1 1 1 1 I 1 12 1 1 I 1 I 1 1 1 r 1 1 1 13 1 1 1 I 1 1 1 1 l I 1 1 14 1 1 1 1 1 1 1 1 l 1 1 1 15 1 1 1 I 1 1 1 1 1 1 16 1 1 j 1 1 1 1 1 l 1 1 1 17 1 1 1 I 1 1 I 1 l 1 1 1 18 1 1 1 1 1 1 I 1 l 1 1 1 19 1 1 1 1 1 1 I 1 x 1 1 1 1
10 3 3 3 1 1 1 I l 1 1 1 1l i 3 3 3 3 1 1 1 1 i t 1 i 112 3 3 3 1 1 1 1 i I 1 1 113 3 3 3 3 1 1 1 1 l 1 1 1 I14 1 1 1 1 1 1 1 1 i 1 1 1 115 1 1 1 1 1 1 1 2. l 1 1 1 116 1 1 I 1 1 1 I 1 l 1 1 1 I
" 1 7 ” 2 2 2 2 2 2 2 2 2 2 2 2 218 2 2 2 2 2 2 2 2 2 2 2 2 219 2 2 ? 2 2 2 2 2 2 2 2 2 220 2 2 2 2 2 2 2 2 2 2 2 2 2
FISSION SOURCE DISTRIBUTION AND SUM 1.00000 0 .0 ________ 0 .0________ 0^0________ 1.00000
PERTURBATION INPUT - SECTION 0400 0 0 - 0 0 0 0 0 0 0 0 0 C.O 0. 0 Or.'
C O W SmUGTblFFMMCe 1 wDW5TF40 STlTfa ' CO N5UTIT5 " 17 CT TiKTfeAo c f 'S To rE d -----------T659
Quit ION CONSTANTS Hi LU GE STORED IN COR?
NIIHEEK OF— -COLUMNS; ~KOYttY T T f iK E SY 'Cg OpP5.'~Ur SCATY 'OU.iNSGM ; RETSI O t e V W Z u n e S------------- 13— 20---------------------------------------------- 1----- 4------------0------------0------------5------------3
MEMORY LOCATIONS RESERVE!) FOH DATA STORAGE------ 4(5OCCMEMORY LOCATIONS USED FOR THIS PROBLEM------------- 8SS4UEMORY LOCATIONS NOT USED---------------------------------- 31006
* * * * * * * INT>UT SPtC lfIfcD UPSCATlER = 0 HAS BEEN CHANGED Ttl ACTUAL UPSCATTER = 1
— fRPUT S P t L T F l t D DUWR'SCETTE'S~=— 0— RffS~ETEK"CHCTiS'ED T E ~ ^ U * r ~DCHTr e a T T T ff~ — T
R-Z CASE TO CflMPARE WITH THETA-R -Z CASF, WITH BLACK ABSORBER13X20X4 GROUP, 1040 POINTS STREAM OF CITATICN CASES
LINE RELAXATION WILL BE DONE ON ROWS - 1 INNER ITERATIONS!OFNL 72
ITERATION1
FLUX CHANGE 3.12299E-01
BETA1.00000
MU-10.62460
MU-2-0 .3660b
MU-30 .0
K0 . 38d723
2 -7 .77383E-01 1.84153 -3 .24560 -2 .86353 0.083b6 0.4384373 -7.22449E-01 1.72 641 0.21290 0.59021 0.60952 0.46d0174 8.44198E-01 1.65142 -0 .32432 -3 .25641 0.66200 0.4863515 8 .55601E-0I 1.60598 1.86911 0.25655 0. 71798 0,49$03L6 4.41313F-01 1.57964 0.95711 0.39634 0.72b76 0.50&V157 -2.40255E-01 1.56476 -0 . 78467 -0 .39082 0.59875 0.511456a -2 .701516—01 1.55648 0.8542 8 0.44J22 0.53446 0.5164379 1.68539E-C1 1.55192 -0 .45533 -2 .99261 0.23721 0.519092
10 - I.3 9 4 1 2 E -0 1 !■>. 54941 -0 .96659 -0 .67724 -1 .20965 L>. 52074711 - 9 .84510E-02 1.54803 0.60773 0.31132 2.19028 0.52146312 -7.60495E-02 1.54728 0.69641 0.95159 1.38883 0.52148313 -6 .H 4 7 5 E -0 2 1.54686 0.74290 0.92V97 1.18325 0.52106314 -4.96933E-02 1.54664 0. 76299 0.88406 1.00322 0.52034115 -3.99801E-02 1.54652 0. 76456 0.87122 1.03115 0.51937416 -3.23465E-02 1.54645 0.77672 0.90900 1.00793 0.51828817 - 2 . 77042E-O2 1.54641 0.82878 0.94231 0 . 9341U 0.517119Is - £ » 30943E-02 l.$ 4 6 3 9 0 .Si 051 0.91675 0.98183 0.51587019 -1.68281E-C2 1.5463 8 0.71184 0.87562 0 .961 jO 0.51458220 -1.39726E-02 1.54638 0.81634 0.84447 0.95217 0.51331521 -1.36354E-02 1.54637 0.96223 C .83298 0.96159 0.51207522 7.87067E-C3 1.54637 -0 .56935 -0 .80305 0.96000 0.510U1823 - 7 . 10750E-03 1.54637 -0 .91014 -0 .90388 0.93294 0.50960824 -6 .6734bE-03 1.5*517“ 0 . t)6/ 60 0.92757 U. 50845825 -6 .21027E-03 1.54637 0. 9243 9 0.87515 0.92537 0•50737426 -5 .81551E-03 1. i>4637 0.93062 ' 0 .94356 0.92459 0.50635427 -5 .44858E-03 1.54637 0.93146 0.93946 0.92246 0.50539928 -5.10019E^03 1.54637 0.93096 T . 93835 0.91969
— 7.3678 BE—02 EXTRAPOLATION WITH 14.3735 0.49144 1i.9 S T O lS b iE -^ 1.00000 - 0 . 7U2B3 —0.4/090 14.28070 0.49149630 3 . 91960E-03 1.5463 7 0.98063 1.13537 -0 .01828 0.49160631 3 .70S62t-03 1.54637 0. 94896 1.01221 1.04591 0.49175232 3.12233E-03 1.54637 0.84585 0.94305 1.00630 0.49191733 2.44713E-03 1.54637 0. 78620 0.89847 0.98119 0.49209134 1.80531E-03 1.5463 7 0. 73953 0,88775 0.97811 0.492276T5 -1 .5 0 6 8 7E-03 1.54637 -0 .83619 -0 .7 ^ 757 0.96522 0.49246536 - 1 • 33598E-03 1.54637 0.88526 0.78567 0.95864 0.49265237 -1 .13374E-03 1.54637 0.84749 0.96520 0.94977 0.492o3538 - I . 104776-03 1.5463 7 0. 97334 0.96384 0.94647 0.49301339 -9.36985E-04 1.5463 7 0.84719 0.97 384 0.94035 0.49318540 8.64983IT-04 1.54637 -0 .92229 -0 .92609 0.93540 0.49334841 i . 354146-64 1.5463 7 0.96666 0. (5^039 0.93147 0.4935034? 7.97272E-04 1.5463 7 0.95514 0.947C9 0.92773 0 . 493049■♦3 7.55310F-04 1.54637 0. 94812 0.94S38 0.92420 0.49378544 7.O8580E-04 1.5463 7 0.9388 4 0.94256 0.92093 0.49391345 6.65665E-04 1.5463 7 0. 94010 0.93508 0.91970 0.49403146 6.23703E-04 1.54637 0. 93759 0.93141 0.91765 0.49414047 5786788^-04 1.546*7 ■ 0 .9 T 1 7 7 1 6. $2681 0.91525 0.49424148 5.35011F-04 1.54637 0. 92172 0.97413 0.91206 0.49433449 4.96864E-04 1.54637 0.92920 0.96258 0.91264 0.49441950 4.-59671E-04 1.5463 7 0.92560 0.95314 0.91C41 0.49449751 -4 .27902E-04 1.54637 ~'b'. 9T13T" —0.93fc53 0.90909 0.49456852 -•4.02153E-04 1.54637 0.93942 0.91931 0.90781 0.494634S3 -577*6235-04 1.5463 7 93367 6. 91*C2 0.90661 0.49469354 -3 .49104E-04 1.54637 0.92904 0.91476 0.90556 0.49474755 -3 .22819E-04 1.54637 0,92438 0.91550 0.90462
-3.70406E-03 EXTRAPOLATION WITH 11.4911 0.49535 7' 56 5.14984E-05 1.00000 -0 .15948 -0 .10027 11.44253 0.49t>354
57 5.91278E-05 1.5463 7 1.14821 1.70911 -0 .01698 0.495346
H■P*
— 3
5fl 6.0081 5E-05 1.54637 1.01619 0.90904 0.96Cd4 0.49533859 5.72205E-05 1.54637 0.95244 0.91021 0.94214 0.49533060 5.3405 8F-05 1.5463 7 0.93339 0.91264 0.93135 0.49532361 4 .9591 lE -r 3 1.54637 0. 92862 0.91817 C .93207 0.495316b? 4.67300E-05 1 .54o3 7 0.94235 0.91593 0.92068 0.4953L'963 4 .38690E-05 1.54637 0.93 882 0.91924 0.92058 0.49530364 4. 00543F-r'5 1•54637 0.91308 0.92013 0.91187 0 .49525765 4.00543F-05 1.5463 7 1.00004 0.93273 0.912 39 0.49529166 3 .62396C-05 1.5463 7 0.9048 0 0.92708 0.90599 0.4952dG
ENO fIF err.FNVALUE CAl CUL4 TICN - ITERATION TIME 0.127 MINUTES
CONVFRGFNCE INDICATION RV m in im iz in g JHI SUM UF THE SUUARES CF THE RESIDUES - RELATIVE ABSORPTION 0.9992194 K 0.4953631
LEAKAGE 5.35457E 13 TOTAL LOSSES 1.38698E 1 4 TOTAL PRUDUCTIONS 6.B6952E 13 REACTOR POhERtwATTS) 6.8000UE 07
ADJMINT PROBLEM FOLLOWSITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3
1 3.89566E 28 1 .OGOOO********** -0 .05636 0 .0 0.4952862 9 .033S2fc 00 1. 84153 9.03352 22.45157 0.0 0.495286■a 4.92919E 00 I . 72641 5.47484 0 .2305 6 0 .0 0.4952864 1.98464E 0 0 1.65142 2.38727 0.37429 0 .0 0 »4952o65 9 .67230E-01 1.60598 1.45459 0.44889 0 .0 0.4952866 5.87255E-C1 1.57964 1. 19441 0.59138 0 .0 0.4932807 3.82845E-01 1.56^76 1.03477 0.60607 0.0 0.49528b8 2 .91459F-01 1.55648 1.05276 0.96810 0 .0 0.4952869 2•67919E—A 1 1.55192 1. 1S7I5 0.60590 0 .0 0 .4 95 2d6
10 2. 55519 F -0 1 1.54941 1.20 924 0.80359 0 .0 0.493286l i 1.58237E-01 1.54 803 0.77752 0.83653 0.0 0.495286l? 1.21853E-01 1.54728 0.89192 0.85377 0 .0 0.495286B l.d7 6 4 7 £ -0 t 1.£4686 0 .99l06 0 .8 7 4 9 i 0 .0 0.49528614 9.34916F-02 1.54 664 0.96199 0.89369 0 .0 0 .4v52d615 7.96766F-0? 1.54652 0.93191 0.90408 0 .0 0.495 ?8616 6.82545E-02 1.54645 0. 92490 0.91834 0 .0 Q.4952U617 5 .91P40F-02 1.54641 0.92535 0.95033 0 .0 0 .49520618 5 .15862E-02 1.54639 0.92409 0.92420 0 .0 0.49528bf9 4.47426E-P2 1.54 638 0.91208 0.89534 U.O 0.49528620 3 .86534E-02 1.54638 0.90256 0.89904 0 .0 C ,4952d621 3.34101E-02 1.54637 0.89776 0.93451 0.0 0.49528622 2.93875E-C2 I . 54637 C. 90899 0.884C9 0 .0 0 .49520623 ? . 63290E-02 1.54637 0. 92226 0.86278 0 .0 0.49528624 -2.-26966E-02 1.54637 -0 .88473 -0 .85638 0.0 0.49528625 -2 .01604E-02 1.5463 7 0. 86809 G.8715C 0 .0 0.49528626 - 1 . 78810E-02 1.5463 7 0.86906 0.86344 0 .0 0 . 49528627 -1 .58452E-02 1.5463 7 0. b7U3 0 0.85 857 0 .0
-1.02662E-01 EXTRAPOLATION WITH 6.3766 0.49528628 -3 .95775E-03 1.00000 0.24582 0.15055 0 .0 0.49528629 -4 .94736P-03 1.54637 1.24510 1.39847 0 .0 0.4952d630 -5 ,06425E-0 3 1.5463 7 1.61856 0.87562 d .(T 0 . 49528o31 -4 .9 3 1 2 1E-0 3 1.54637 0.96880 0.93771 0 .0 0.4952863? - 4 . 53097E-0 3 1.5465• 0.9143 0 0.94 701 0 .0 0 .49528633 -4 .0 7 958E-03 1.54637 0. 8963 0 0.857 79 0.0 0.49528634 - 3 . 64506E-C 3 1.54o?7 0.88984 C .82613 0 .0 0.49&28635 -3 .2 4 6 2 5F-03 1.54637 0.88 734 0.90146 0 .0 0 . 49528o36 — 2 .76411E-0 3 1.5463 7 0. b4871 0.85951 0 .0 0.49528637 -2 .68090E-03 1.54637 C .96722 0.88042 c .o 0.49528638 -2 .2 4 8 ? 5E-0* 1.54637 0.83 b41 C .87909 0 .0 0.49528O39 -1 .9667 IE-03 1.54637 0.87277 0.88263 0 .0 0.49520640 - 1 . 7843 8F-03 1.54 63 7 0.90551 0.88184 0 .0 C .4952d641 -1 .65141E-03 1. 54637 0.92333 0.88026 0 .0 0.495286
-1 .520286 -0 ‘i 1•54 63 i 0.9190? (5.87424 0 .0 0.4y52d643 -1 .3 9 1 71E-03 1.5463 7 0.91404 0.87484 0 .0 0 . 4952o644 — 1. 26576E-03 1. 54 63 7 :i.90d24 0.88429 0 .0
-1.09419E-02 EXTRAPOLATION WITH 8.6396 0.49528645 2•09808E-04 I . 00000 -0 .16555 -0 .26821 0 .0 0.49528646 2 .77519E-04 1.54637 1.32300 1.44376 0 .0 0.49528 6
4/ H L 334fc—U 4 1.5465 t 1.01403 U.906CJ0 0 .0 0.49520648 2.77519E-04 1.54637 0.98672 0.88320 0 .0 0.4952S649 2.6130 7F—04 1.54637 C .94184 0.89611 0 .0 0.4952.1:50 2 .38419E-04 1.5463 7 0.91265 0.89914 0 .0 0.49528653 2 . 14577F-04 1.5463 7 0.90021 0.90124 0 .0 0 . '1952865? 1.92642E-C4 1.54637 C-. 8979 7 0.9C 6 53 c .o C .49526653 1.64 986E-04 1.54637 0 .8 5 6 6 0 0.90715 0 .0 0.49528654 1.602176-04 1.5463 7 0.97126 0.91045 0.0 0.49528655 1 .35422E—0 4 1•5463 7 C .84537 0.91405 0 .0 0.49528656 1. 18256E-04 1.54637 0.87336 0.91954 0 .0 0.49526657 1.0395 IE-0 4 1.54637 0.87914 0.94395 0 .0 0.49528658 9 .05991E-05 1.5463 7 0. 87165 0.92815 0 .0 0.495286
END OF APJOINT CALCULATION - ITERATION TIME 0.075 MINUTES
CONVERGENCE INDICATION BY MINIMISING THE SUM OF The SQUARES OF THE RESIDUES - RELATIVE A6SGRPTI0U 1.0011587 K 0.455530*
GROSS NEUTRON BALANCE
GRP LFT LEAKAGE TOP LEAKAGE RIT LEAKAGE BOT LEAKAGE FNT LEAKAGE 8AK LEAKAGE B**2 LOSSES 1/V LOSS XENON LOSS1 C.O " 6 .0 1 • 64306E i ' i 2.12991E 12 0 .0 0.0 0 .0 0 .0 0 .02 0 .0 0 .0 5.S7573F 12 1.67591E 12 0 .0 c .o O.C 0 .0 0 .03 0 .0 0.0 2.97323F 12 9.17628E 11 0 .0 c .o 0 .0 0 .0 c . o4 0 .0 o .c 1.69606E 13 6.48216E 12 0 .0 0 .0 0 .0 0 .0 0 .0
SUM 0 .0 0 .0 4.23401E 13 1.12056E 13 0.0 0 .0 0 .0 0 .0 0 .0H-P*
GRP1
ABSORPTIONS 5.20004E 12
OUT-SCATTER 1.14916E 14
SOURCE1.3<J698E 14
IN-SCATTER0.0
TOTAL LCSSES 1.3 8t>77E 14
TCTAL GAINS 1.3db9dE 14
PROD/ABSCRP 3 . 65590E—01
23
1•?3 706E 13 8.49 695F 12
9.4fc847E 13 8.?6228E 13
0 .0v.c
1.1491tfc9.50156E
1413
1.14907b9.50106E
1413
1.14916E9.5C156E
1413
4.00152E-013.55114E-01
4 5.90 H 7 B 13 1.50&MS 11 ~6.d ti.'J&FS'eE 13 8.2b583E 13 8.2o22BE 13 9.9563 IE-01
Sum 8.5J523E 13 2.9 25546 14 I.38648E 14 2.92554E 14 4.31252E 14 4.31252E 14
tuNF AVERAGF POWER 6.89-»33E 02 0 .
UL IVSl f ItSIWA 1 1 S/tC 1 0 0 .0
THE MAXIMUM POWER DENS I TV( WATTS/CC) AT ROW 16 AND CCLUMN 9 IS 7.599082E 02
THE AVERAGE.POWER DENSITY ALONG RCW 16 IS 7. 353403E 02 AND THr. RELAT1VE PQWEK DENSITIES!FRACTION OF AVERAGE) ARE8 . 5 9 2 1 0 3 F - 0 1 1 . 0 3 0 9 1 2 F 0 0
8 . 8 0 5 4 7 6 F - 0 1 . 1 . 0 5 4 7 6 1 E 0 0
. 9 . 0 1 2 56 I E —C l 1 . 0 1 6 0 0 2 E 0 0
9 . 2 1 2 5 3 7 u - 0 1 1 . 0 0 5 5 8 5 E 0 0
9 . 6 0 9 6 1 2 E - 0 1 9 . 9 9 d 2 1 0 E - 0 1 1 . C 2 C S 6 C E 00 1 . O 3 0 8 U 4 E 0 0 l i 0 3 3 4 i 0 E 0 0
T H E A VERAGE POWER D E N S I T Y DDWIV1 COLUMN 9 I S 7 . 0 7 8 4 7 7 E 0 2 ANC T H E REIL A T I V E POWER D E N S I T I E S AREJ i . 0 0 7 6 8 8 E 0 0 - 9 . 7 3 7 1 4 7 c — 01
1 . 0 0 6 U 7 E 0 0 9 . 781 54 OF — 01
i . a o s s t b P 609 . 6 83 5 7 7 E - 0 1
9.^87614E-01 1.004636F JO
9.934847E-01 1 .C25369E 00
9 .8/6527c-01 I.047J.41E 00
9 .d l9B 49E -0 I 1.07354 7E 00
9.771283E-C1O.C
9.740434E-U10 .0
H - i COSE K ) COtPftDf WITH T H g T a ~ a » * CASE . WITH frtftC* ABSby.Hta______________T f f H T f ' T S o u 0 , l o ^ o T o T S T s ~ " s ( s t am c>t- c i t s t j o n c a s f s u».-vt 72
m r o n r j v r d n r w s w .r s - - " T/"•'£f hh£HE S ScHjjtiehifs CKOSi S K lid A l* . LAMB0AIPH1 * M PH I) = 1 . 1-.3320E-G5
CGM*5 W W l: " GWP SIGR »Dil**2 ViU*SlG? 01 FF. C O tf. 6**21 CCKF 7ONE i I -1.59JOOSE 02 3f iJ42B?E 0^ -6 .416064E-03 -? «a b lJ 8 2 £ 02
? -S.SHOSrBS1* 01 ^ .04 f6 lfcE 62 -9 .2 2 4 9 2 U -0 3 -b .'#e*423£ 013 -3 ,513637? C5. 5».07ZCeZE CX - 7 . J47491E-05 -t>*CS08 M*. C l4 - 2 . 0 9 5 ^ $ f Sz D W J I J T 02 ~ 3 • V 2 S a i v t -0 2 '3 »M 2r.9 ;)E 02
a c o r f ;o f » f 2 1 -1.8G712GE Oi 3.64S6Q1E QX - i .S 'i t t i j i z t - a a - 'i» fc 6 o ir *E ClX -3 .327V02E 01 2,4&7aatE <5i - i .b«7Ja«5SK-C) -i*17.<i*iaE O’3 — 7*6007? 3c Oft K277619E .01 -6.75b34ttE-.34 " 0 . ?b34u2c y j4 - ? .3 fsYoafc e i 3 . m * i u Oi 4.t?C42edt-03 -4 .b2322 fE 0-i
3 4 If IM . a tK f 1 1 o*n u .o 0 -0 0.02 1 M ,l r c . o 0.0 0.03 o .c S5.0 0*0 0.0
d .6 u .a 0 .0 0«u
'• u 'yp W A ffr ...... T R V 7 t — • " " T T s r r r s s s " a1 t v z v . ■' j t s m r 1 c s p « if r1 CORt IONS l I 1.S-S2009E 02 5 , lS d 7 * 7 £ 0 { 2 « S 1 ^ U 7 £ U l I . U O c i i i c 02
p 1.94735:>E C2 6 . ‘330^83 fe CX 3.C&14VCI: O l 1 . 0 2$(»34{: 023 .*i2»*935E 02 7 .2 6 3 6 5 5 6 01 A .5 1 3 3 ? 7 £ O i i.e&bS^'jfc u?4 2.5 1 6 0 5 * 5 02 8 .1 6 3 4 C 8 E o l 3 .9 4 3 3 1 4 6 01 i»u 9 a ii3 S E 02
2 CORE ZONE 2 1 1.807120E 01 :;* 9 2 6 C 2 E C l 6 .3 2 7 9 3 3 E 30 4 .3 2 ? i«»2 E 01"" J 2.<Sl4252E 61 1 T 7 ^ 2 ^ v 6 2 t $1 7 . 0 4 5 3 2 I E uO 4 , & i ? U 2 E o l
3 2.176309E 01 1.432929E 01 7.-*9QL7 23F 00 &.195534E 014 2 . i 5 6 7 3 9 E 01 1 .4 8 3 8 1 tE 01 ? .8 6 7 7 6 9 l * > 5 .37570SE Oi
3 AXIAL BLKT 1 1 0 . 0 0 .0 0 . 0 ______i 0 . 0 0 . 0 "576 ■ 0 . 0 '3 0 . 0 0 .0 0 . 0 0 .04 o . 6 6 . 0 6 . o 0 . 0
END OF C A S r ^ T ( i r 4 L C<>0 “ IMe was d. 25 MINUTES TOTAL CLOCK TIME: WAS 1 .4 4 MINUTES♦ I*********************************************************************t»********.> ******************************
*»♦ <■*»*♦ *! H is JOB MA5 RUN ON— C T= TT= 7 2 — CN T H F I b M 466741*********
T H E T A -R -Z CASE WITH BLACK ABSORBER, PERIODIC4X13X20X4 GROUP, 4160 POINTS STREAM OF C I T A T I O N CASES OHNL 72
GENERAL CONTROL INPUT - SECTIO N 001
0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 I 0 0 0 C 01 0 0 0 I 0 0 0 1 0 O i l 0 0 0 0 0 U 0 0 0 0 0
. 160 i o o i o i 3 c o 0 0 0 0 0 0 0 0 0 0 0 12 6 12 6 12 241 . OOOOOOE 02 9 . 9 9 9 V 9 9 E -0 5 9 .9 9 9 9 9 9 E 09 9 .9 9 9 9 9 9 E 23 0 . 0 1 . OOOOOOE 00
NEUTRON FLUX PROBLEM D ES C R IP TIO N - SECTIO N 003
0 0 0 0 12 0 0 0 0 0 - 1 1 - 1 0 1 0 3 0 0 0 0 C 0 09 .9 9 9 9 9 9 E - 0 5 l .O O O C C 0 E -0 5 9 .9 9 9 9 9 9 b —05 9 .9 9 9 5 9 9 E —05 9 .9 9 9 9 9 9 E— 05 0 . 09 .9 9 9 9 9 8 E -0 3 - 4 . OOOOOOE 00 6 .8 0 0 0 0 0 E 01 l.UOOCOOE 00 1 . OOOOOOE 00 0 . 0
L E F T ,T O P ,R I G H T ,B O T T O M ,F R O N T .B A C K BOUNDARY C O N D IT IC N S AREP E R IO D IC 0 . 0 P E R IO D IC 9 .9 9 9 9 S 8 E -0 3 0 . 0 9 .9 9 9 9 9 8 E - 0 3
HOB BND. 'CONSTANT5 m ZONE— 5-----------------------------------------------------1 . 5 2 6 0 0 0 E -0 2 7 .4 5 3 9 9 6 E -0 2 1 .1 0 2 3 0 0 E -0 1 1 .2 '4 2 0 9 9 E -0 1
THREE DIMENSIONAL C Y L IN D R IC A L GECMETKY I R , T H E T A , Z > WIDTH 6 .2 8 3 I B 6 E 00 H E IG H T 3 . OOOOOOE 01 DEPTH 4 .5 9 9 9 9 8 E 01
REGION S P E C IF IC A T IO N S P TS REGION WIDTH
4 6 .2 8 3 1 8 6 E 00
P TS REGION HEIGHT— s ~ ? T s r o o o o E ~ o i ---------------9 "~g .o a o o o g g c i
PTS REGION DEPTH9 2 . OOOOOOE 01 4 1 . OOOOOOE 01 3 6 . COOOOOE O o 1 . COOOOOb 01
X - D I R . POINTS 4 Y -D I R . P O IN TS 13 Z -D lf i . POINTS 20
DISTAN CES TO 1HESH INTERVAL IN TER FA C ES
J D I S T .2 1 .5 7 1 3 . 3 .1 4 2 4 4 .7 1 2 5 6 . 2 8 3
1 U 1 1 .2 5 .0 0 0 3 7 . C71 4 8 .6 6 0 5 1 0 . 0 0 0 6 1 3 .7 4 4 7 1 6 .6 6 7 a 1 9 .1 4 9 9 2 1 .3 4 4 10 2 3 .3 3 3
11 2 5 .1 6 6 12 2 6 .8 7 4 13 2 8 .4 8 0 14 3 0 .0 0 0
kft C I S T 2 2 . 2 2 2 3 4 .4 4 4 4 6 .6 6 7 5 a. 869 6 1 1 . 1 1 1 7 1 3 .3 3 3 8 1 5 .5 5 6 9 1 7 .7 7 6 10 2 0 . 0 0 0
11 2 2 .5 0 0 . 20 4 3 .5 0 0
1221
2 5 . COO 4 6 .0 0 0
13 2 7 .5 0 6 14 i b . o c o 15 3 2 .0 0 0 16 3 4 .0 0 0 17 3 6 .0 0 0 18 3 8 .5 0 0 19 4 1 .0 C 0
DISTANCES TO FLUX PO IN TS
1 0.785 2 2.356 3 3.927 4 5.498
I D J S T .1 3 . 5 3 6 2 6 . 1 2 4 3 7 . 9 0 6 4 9 . 3 S 4 5 12. 01 9. 6 1 5 .2 7 5 7 1 7 .9 5 1 8 2 0 . 2 7 6 9 2 9.361
10 2 4 .2 6 7 11 2 6 . 0 3 4 12 2 7 . 0 8 9 13 2 9 . 2 5 0_ _ =
1 1 . 1 11_____ 2 3 . 3 33______3____ 5 . 556 4 7 . 7 7 B 5 1 0 . 00 0 6 1 2 .2 2 2 7 14.444 8 1 6 . 6 6 7 9 18.88910 2 1. 25 0 11 2 3 . 7 5 0 12 2 6. 25 0 13 2 8 . 7 5 0 14 3 1 .0 0 0 15 3 3 . 0 0 0 l o 3 5 . 0 0 0 1/ 3 7 . 2 5 0 18 3 9. 75 019 4 2 .2 5 0 20 4 4 . 7 5 0 ________ ________________________________________________________________________________________________
ZONE INPUT BY REGION
PLANE NUMBER 1 1 1
PLANE NUMBER 2 3 1
PLANE NUMBER 3 11__________
PLANE NUMBER 42
ZONE NUMBER AT EACH MESH INTERVAL VJ1--------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------ro
S P E C I F I C A T I O N FOR LAYFR NUMBER I
1 2 3 4
1 1 1 1 12 1 1 1 13 1 1 1 1 '4 1 15 1 1 1 16 1 1 1 17 1 1 1 18 1 1 1 19 1 1
10 1 1 1 111 1 1 1 112 1 1 1 113 1 1 1 1
i P E C ! F I C A T ION FOR LAYER NUMBER 2
1 2 3 4
1 1 1 1 12 1 I 1 1 ' "3 1 1 1 14 1 1 1 15 1 1 I 16 1 1 1 17 1 1 1 1
8 1 1 19 1 1 I
10 1 1 111 1 1 112 1 1 113
S P F C IF I ATION FOR LAYFR NUMBER 3
1 2 3 4
1 1 1 1 12 1 1 134 1 1 I5 1 1 16 1 1 17 1 1 1e 1 1 19 1 1 1
10 1 1 1 ' -1112 r " T 1 ' T ..... ........................... '13 l l l
SPFCIFI ATION FOR LAYER NUMBFR ^
1 2 3 4
1 1 1 1 12 1 1 134 " 1 1 " T -------- --------- -------- '56 1 1 17 1 1 169
l o i l i11 l l l12 l l l13 1 1 ' !■
SPECIFICATION FOR LAVER NUMBER 5
1 2 3 4
1 1 1 1 12 1 1 r3 1 1 14 1 1 15 1 1 16 1 1 17 1 1 16 1 1 19 1 1 1
10 1 1 111 1 1 1
’ 12 1 1 113 1 1 1
HVJ1U>
SPECIFICATION FOR LAVER NUMBER 6
1 2 3 4
1 1 1 1 12 1 1 1 13 1 1 1 14 1 1 1 15 1 1 1 16 1 1 1 17 1 1 1 18 1 1 1 19 1 1 1 1
10 1 1 1 1l i 1 1 1 112 1 1 1 1 '13 1 1 1 1
SPECIFICATION FOR LAYER NUMBER 7
1 2 3 4 _____________________
1 1 1 1 12 t i l l3 1 1 1 14 1 1 1 15 1 1 1 16 1 1 1 17 1 1 1 18 1 1 1 19 1 1 1 1
i o 1 "1 1 111 1 1 1 112 1 1 1 113 1 1 1 1
SPECIFICATION FOR LAYER NUMBER 9
1 2 3 4
1 1 1 1 12 i i 1 l3 l l l l4 i i l l5 l i l l6 i i l l7 l 1 1 I6 1 i l l9 l 1 1 1
10 1 i l l11 l i l l12 l T ” I l ’13 l 1 1 1
SPECIFICATION FOR LAYER NUMBER 9
1 2 3 4
1 1 1 1 12 1 1 1 13 1 1 1 14 1 1 1 15 1 1 1 16 1 1 1 17 1 1 1 13 1 1 I I9 1 1 1 1
10 1 1 I I11 1 4 1 112 l i l t13 1 1 1 1
SPECIFICATION FOR LAYER NUMBEK 10
1 2 3 4 ______
1 3 3 3 32 3 3 3 33 3 3 3 3T ' I 3 I 35 1 1 1 16 1 1 1 1T 1 1 1 18 1 1 1 19 1 1 1 1
15— I I I T 11 1 1 1 115 I 1 1 113 1 1 1 1
SPECIFICATION FOR LAVER NUMBER 11
1 2 3 4
1 3 3 3 31 — i r 3 i3 3 3 3 34 3 3 3 35 1 1 1 16 1 1 1 17 1 1 1 1ft 1 1 1 19 1 1 1 1
10 1 1 1 111 1 1 1 112 1 1 1 113 1 1 1 1
SPECIFICATION FOR LAVER NUMBER 12
1 2 3 4
1 3 3 3 32 3 3 I 33 3 3 3 34 3 3 3 35 I I I I
Hv nv n
6 1 1 1 17 1 1 1 18 1 i l l9 1 1 l l
i o 1 i l l11 1 1 l l12 1 i l l13 1 1 1 1
SPECIFICATION FOR L4YF.R NUMBER 13
1 2 3 4
1 3 3 3 3? 3 3 3 33 3 3 3 34 3 3 35 1 1 16 1 17 1 1 18 1 1 19 1 1 1
1* 1 1 111 1 1 112 I 1 113 1 1 1
SPECIFICATION FOR LAVFR NUMBER 14
»-• rv>
1 1 i
i 1 1 1 12 " ' T 1 T " T ........""3 1 1 1 14 l l l l5 1 1 1 16 1 1 1 17 l l l l8 ' T 1 " T " 1 ........9 l l l l
" i o ' T 1 "1 " T "l i l l l l
~ n l l l l13 l l l l
SPECIFICATION FOR LAYER NUMBER 15
1 2 3 4
1 l l l l2 1 1 i i ............. "3 l l l l4 " 1 1 T 1 ......................5 l l l l6 ■' V 1' T 1------ -------- ----------7 l l l l8 l l l l9 l l l l
10 l l l l11 l l l l
Hv nCT\
12 1 1 1 113 1 1 1 1
S P E C IF IC A T IO N FOR LAYER NUMBER 16
1 2 3 4
1 1 1 1 12 1 1 1 13 1 1 1 14 I 1 1 15 1 1 1 16 1 1 1 17 1 1 1 18 1 1 1 19 1 1 1 1
10 1 i r 1 '11 1 1 1 112 1 1 1 113 1 1 1 1
SPECIFICATION FOR LAVER NUMBER 17
1 2 3 4
1 2 2 2 2i -------- 5” 2 r I
3 2 2 2 24 2 2 2 25 2 2 2 2
“ 6 2 2 2 27 2 2 2 2
“ 3-------- 2 2— 2— ?9 2 2 2 2
TO 2 2 2 211 2 2 2 ?12 2 2 I 213 2 2 2 2
SPECIFICATION FOR LAVER NUMBER 18
1 2 3 4
1 2 2 2 22 2 2 2 23 2 2 2 2
“ 4 2 2 2 F5 2 2 2 2
“ 5-5 2— 2— ?7 2 2 2 28 2 2 2 2"9 2 2 2 2
10— 2 2 2 211 2 2 2 212 2 2— 2 ST1? 2 2 2 2
SPECIFICATION FOR LAYER NUMBER 19
1 2 3 4
1 2 2 2 22 2 2 2 23 2 2 2 24 i 2 £ 25 2 2 2 26 2 2 2 27 2 2 2 28 2 2 2 29 2 2 2 2
to 2 2 J 211 2 2 2 212 2 2 2 213 2 2 2 2
S P E C IF IC A T IO N FOR LAYER NUMBER 20
1 2 3 4
1 2 2 2 22 2 2 2 23 2 2 2 24 2 2 2 25 2 2 2 26 2 2 2 27 2 2 2 28 2 2 2 29 2 2 2 2
10 2 2 2 211 2 2 2 212 2 2 2 213 2 2 2 2
PFRTURBATION INPUT - SECTION 0400 0 0 0 0 0 0 0 0 0 0 0 0 .0 0 . 0 0 . 0
Core s to ra g e d i f f e r e n c e (w o rd s i e q u a tio n co n s ta n ts i/ o in s te a d o f s to r e d 12577
F SU T m ilN £ 0 N 5 T £ N T 5 WIl L 'B E STORED "IK rG RE '■ " "
NUMBER OF-------COLUMNSt ROWS, PLANES, GROUPS, UPSCAT, OOWNSCAT. REGIONS, AND 1DNES 4 13 20 4 1 1 8 3
Memory LOCATIONS RESERVED POE C 5 T J STORAGE------ 40Cfi0 ”MEMORY LOCATIONS USED FOR T H IS PROBLEM----------------- 28330MEMORY LOCATIONS NOt USED—---------- ---------------------- 11670
TH C TA-R-Z CASE WITH BLACK ABSORBER. P E RI O DI C4*13X20X4 GROUP* 4160 POINTS STREAM OF CITATION CASES ORNL 72
LINE RELAXATION HILL BE OONE ON ROWS - 1 INNER IT E R A T IO N SITIftXTTtoN FLUX tH A N b t b e T a MU-1 HU-2 MU-3 K
1 1.45619E-61 I . 00000 0.29004 -0 .2 0 6 2 9 0 . 0 0 .3 8 1 5 6 42 6.42240E-01 1.78515 5.07091 4.83015 0.03961 0 .4084573 -4 .‘ 01546E-01 1.64630 -1 .02677 -0 .20579 0.72106 0.4243794 -3 .19332E-01 1.56750 0.47592 0.77797 0.81176 6.4359855 -2 .52715E-01 1.52605 0.5386 7 0.779C5 0 .8 6 ? '* 0*4*53956 -1 .98224E-01 1.50511 0.58615 0.75414 0 .902-it 0 . ^ 3 4 7 07 -1 .5 4 8 6 2E-01 1.49475 0 .6 2 6 3 9 0 .8 2 0 4 2 0 .9 1 2 1 4 0.460576a -1 .20348E-01 1.48968 0.65678 0.88927 0.91479 6.4669459 - 9 . 7 5 1 4 2 E - r 2 1.48720 0.71275 0.97079 0.90719 0.472699
10 -8 .13560E-02 1.48600 0.75294 0.97971 0.90082 6.47795611 -7 .08427E-02 1.48542 0.79993 0.98611 0.89604 0.482772
1 2 -6 .28766E-62 1 .4 8 5 1 4 0 .8246C 6.88531 0.88798 0.48718113 -5 .42305E-02 1.48500 0.80834 0.79292 0 .8 8 4 0 9 0.49119514 -5 .08053E-02 1.48493 0.88604 0.87978 0.88059 0.494859IS -4 .76876E-02 1.48490 0.89095 0.87359 0.87447 0.49819716 -4 .50288^-02 1.48489 0.89922 0.93959 0.86712 0.56123417 -4 .39205E-02 1.48488 0.93147 0.97730 0.85764 0.504004i s - 4 . 3 3 1 4 2 E - 6 2 1 .4 8 4 8 7 0.44286 6.98027 0 .8 4 6 0 8 0.50651919 -4 .27014E-02 1 .4 8 4 8 7 0 .9 4 3 1 5 0 .9 7 9 1 0 0.83203 0.50880120 -4 .23434E-02 1.48487 0.94927 0.97824 0.81442 0 .5 1 0 8 6 321 —3 .53847E-02 1 .4 8 4 8 7 0.80028 0.97728 0.79137 0.512711i z ~ 3 . 3 0 6 1 1 6 -0 2 1 .4 5 4 6 ? 0.<*0l2? 6.97716 0 .7 5 9 0 4 0 .5 1 4 3 6 623 -3 .09947E-02 1.48487 0.90650 0.97709 0.70997 6.515839"24 - 2 . 8B<2()8E-62 ' 1.46'487 b . ^ o l o 4 0 . ^ 7 5 4 7 0.62721 6.51714425 -2 .7 6 0 9 0 E-02 1.48487 0. 93034 0.97414 0.45844 6.51829326 -2 .66175E-02 1.48487 0.93747 0.97239 -0 .07336 0.51929727 -2 .5 6 0 3 XE-02 1.48487 0.93629 0.97104 14.28882 0.52016628 -2.46052E-C2 1.48487 0.93642 0.97068 1.84222
—5 . 17821E-01 EXTRAPOLATION Ul TH 20.5276 0.536860' " 2 9 " ' 2 . 74496E-02 1.00000 -1 .08815 -0 .63526 24.34102 0.536175
30 3 .2 2 8 2 8 E -0 2 1.48487 1.20836 1.26730 0 .3 9 1 4 8 0.534379“ 51 3.144651-02 1.48487 1.00554 0.942S8 0.96329 0.532637
32 2 .8 6 8 1 8 E - 0 2 1.'48 487 0 .9 4 0 7 6 0 .9 + 2 2 2 0 .9 5 5 9 9 0 .5 3 0 9 6 2~ 7 i ' 2.55842E-02 1 .4 6 4 6 ? 0.91759 0.92619 0.95470 0.52935434 2 .3 0 6 5 6 E -0 2 1 .4 8 4 8 7 0.9 2 4 6 2 0 .9 2 5 8 2 0 .9 5 4 0 0 0 .S 2 7 8 1 2„ - g j
2 .1 U 7 2 E -0 2 " 1 .4 6 4 6 7 0.93665 0.94630 0 .9 5 3 6 ^ 0.52633236 1.92785E-02 1.48487 0.93221 0.94750 0.95339 0.52491437 1 .7 5 t»0 9 F -0 2 1.48487 0.92529 0.94922 0 .9 5 3 2 5
2.56931E-01 EXTRAPOLATION WITH 14.9380 0 .5 0 2 0 0 33a 4 .7 0 9 2 4 E -0 3 1.00000 0 .2 7 3 8 0 0.59022 15.03033 0 .5 0 2 6 5 539 6.78444E-03 1.48487 1.44745 0.87743 0.01653 0.56226746 6 .3 4 003fc-03 1 .4 » 4 l )7 0 .9 4 0 8 4 6.92665 0.957*7 6.50189541 6.14357E-03 1.48487 0.97516 0.97420 0.94580 0.50154342 5 . 6 6 0 0 6 F -0 3 1.46467 0.92696 "6.93?17 0 .9 4 5 9 6 0.50121043 5.17654E-03 1.48487 0.91975 0.93621 0.94586 0.50089744 4 .9 l7 l4 E -0 3 1 .4 8 4 8 7 0.9 5 4 8 1 0 .9 5 7 6 1 6.94767 0.5 0 0 6 0 145 4.63390E-03 1.48487 0.94703 0*95172 0.94758 0.50032146 4.37064E-03 1 .4 6 46 f Q. 9475 1 0 .9 5 3 9 8 0 .9 4 7 51 0.56005547 4.14562E-63 1.48487 0.95265 0.95626 0.94831 0.49980448 3* 90816E—03 1.45467 0 .^ 4 6 6 3 6 .94966 6.9466T 0 .4 9 9 5 6 649 3.66116E-03 1.48487 0.94046 0.94442 0.94720 0.499340bo 3.44276E-03 l.~454'57 0.94379 0.94630 0.94751 6.49912651 3.24726E-03 1.48487 0.94646 0.94861 0.94764 0.498924
"52 3.04ZZ2E-03 1.46467 0.93990 b . 94136 6 . 44726 0.49873253 2.85435E-03 1.48487 0.94110 0.94505 0.94770 0.498550
”54 2 . 67696E-03 1.46467 0.94053 0.94141 0.947494.25599E-02 EXTRAPOLATE WITH 15.9408 0.495627
35 5.06401E-04 1.00000 0.18968 0.14279 15.98626 0.49562056 6.26564E-04 1.48487 1.23791 1.10857 0.00675 0.495602
VJ1VO
57 6.0176BP-04 1.43487 0.96103 0.88475 0.96723 0.49558458 5.646026-04 1 .4 8 4 8 7 0.97206 0.94990 0,95922 0.49556859 5.45b02E-04 2.48487 0.93366 0.82337 0.95619 0.49555160 5 .102 !66 -04 1.4648 7 C .93582 0.91850 0.9556* 0.495536b\ 4.77791E-04 1.43487 0.93693 0.86516 0.95724 0.49532062 4 .4 4 4 1 2 6 -0 4 1.48467 0.9305 ft 0 .91627 0.95684 0.495506ib3 4 . 10080E-04 1.48487 0.92316 0.95479 0,95322 0.49549264 3 . 7 5 7 4 8 E -0 4 1.48487 0.91665 0.96420 0.95328 0.49547865 3 .4 3 3 2 3 E - 0 4 1.48487 0.91405 0.96117 0.95570
S .1 S 8 7 7 E -0 3 EXTRAPOLATION WITH 15.0286 0.49527366 1.38283E-04 l . o o o r e P . 40292 0.79020 15.10462 0.49527167 -U 1 0805E -04 1.48487 -0 .80140 -1 .12735 0.01966 0.49526768 -1 .0 4 t2 5 E -0 4 1.48487 0.94503 0.91498 0.97350 0.49526469 -6 .94666E-C5 1.48487 0.85421 0.95357 0.98883 0.495260
END OF EIGENVALUE CALCULATION - 1 TERMIGN TIME 0.812 MINUTES
CONVERGENCE INDICATION BV MINIMIZING THE SUM OF THE SQUARES CF THE RESIDUES - RELATIVE ABSORPTION 1.0005999 K 0.4951307
LEAKAGE 5.35521E 13 TOTAL LOSSFS 1.38706E 14 TOTAL PRODUCTIONS 6.86936E 13 REACTOR PONERIWATTS) 6.80000E 07
ADJOINT PROBLEM FOLLOWSITERATION FLUX CHANGF BETA MU-1 MU-2 HU-3 K
1 I •882196 28 l .Q O OO O **1******** ■-0 .03340 0 .0 0.4952602 " I . _421>9E 01 1.78515 14.21786 8.82361 0 .0 0.4952603 7.0723 6E 00 1.64630 7.56979 0.54920 0 .0 0.4952604 3.90246E 00 1.56 750 4.45425 0.73737 0 .0 0.4952605 1.56926E 00 1.52605 1.97139 0.79452 0 .0 0.4952606 1.008786 00 !.50511 1.65162 0.79583 0 .0 0.4952607 6.5842 IE-01 1.49475 1.31111 0.796C3 0 .0 0.495260fi 3 . 2 S 1 M E - M 1.46968 1.07829 6. ?9?01 0 .0 0.4952609 3.288806-01 1.48720 1.09711 0.78444 0 .0 0.495260
10 2.588516-01 1.48600 1.04592 0.78123 0 .0 0.49526011 2.132566-01 1.48542 1.03711 0.92706 0 .0 0.495260I F i .8 0 7 i5 (= -0 l 1.48514 1.02812 0.94193 0 .0 0.49526013 1.560266-01 1.48500 1.01941 0.93551 0 .0 0.49526014 f . 4 6 3 5 8 E - 6 I 1.48443 1.64 4 6.95271 6 .0 0.49526015 1.29909E-01 1.48490 1.05546 0.94889 0 .0 0.49526016 1.21187E-01 1.48489 1.05405 0.95434 0 .0 0.49526017 I . 115806-01 1.48488 1.03230 C .95621 0 .0 0.49526618 1.02804E-01 1.48487 1.02415 0.95456 0 .0 0.49526019 9.46550E-02 1.48487 1.01539 0.94312 0 .0 0.49526026 ...... T .T U 6 5 E -6 2 " 1 .4 S 4 S 7 ' 1.00*40 0.95/43 0 .0 0.49526021 8.07619E-02 1.48487 1.00788 0.93767 0 .0 0.495260'22 ' 7 .$064?t-62 1.48487" 1.00452 6 .^6 3“*6 0 .0 0.49526023 7.02515E-02 1.48487 1.00613 0.96517 0 .0 0.49526024 6.6610JE-C2 1.48487 1.01478 C .96927 0 .0 0 -*9526023 6.3102 76-02 1.48487 1.01044 0.96925 0 .0 0.49526026 5.97639E-02 1 .4 M B 7 ' 1. 0 0 bB 5 0. 96b87 0 .0 0 .4 9 '27 5.65929E-02 1.48487 1.00353 0.96930 0 .0 0 . < ’ .26028 5.359466-02 1.48487 1.00061 0.96911 6 .0 0.49526029 5. 07650F-02 1.48487 0. 99797 0.96930 0 .0 0.49526030 4.80986E-02 1.48487 0.495^7 6.56 '9 i6 6 .6 ' 0.49526031 4.558756-02 1.48487 0.99338 0.97245 0 .6 0.49526032 ' 4 I .3 2 2 5 3 E -6 ' 1•4648 0.991-41 0 . 9 7 T 6 3 ' 0 .0 0.49526633 4.09994E-.I ‘ 1.48487 0.96950 0.97129 0 . 0 0.49526034 3.8908cE-0? 1.48467 d.4a?9b 0.97069 0 .0 0.49526035 3.69349E-02 1.48487 0.98622 0.97016 0 .0 0.49526036 3.5&790F-O2 1.464^7 0. 90483 (3.96946
. . 0 T g ------------ . . . .6."495560
37 3.33290F-02 1.48487 0.98344 0.96889 0 .0"T T 3 2 0 9 6 E 00 " EX IK Ap ULA11UN W1 IH 40.9548 0.495260
38 1 .76868E-02 1.0 0 0 0 0 0.54836 0.60234 0 .0 0.49526039 2.S3210E-02 1.4&487 1.4569& l.4aB '36 0 .6 0.49526040 2 . 36673E-02 1.4U487 0.9563& 0.95119 0 .6 0.49526041 2.220636-02 1. 44148 7 0.96047 0.95178 o .u 0.4952604? 2.09217E-C2 1.48487 0.96 307 0.94964 6 .0 6.495260
43 1.99184F-U? 1.48'.0 7 0.9/197 0.972S0 0 .0 0.49526044 1.89848E-0? 1.48487 0.97211 0.96047 0 .0 0.49526045 1.81236E-02 1.40* 8 7 0.97^76 0.96472 0 .0 0.4952t>046 1.7296 8E-0? 1.48487 0.9/16/ 0.95 926 0 . 0 0 .49326U47 1.65253E-02 1.484b / 0.9/192 0.95902 0 .0 0.49526048 1 • 5Br'43E-C2 1.48487 0.97 218 0.91727 0 . 0 1) .49526U49 F.51014E-0? 1.48487 0. 97003 0.96188 0 .0 0.49526050 1.44596E-02 1.48487 0,97196 0.97544 0 .0 0.49526051 1.38603F-f'2 1 .484b7 C .97298 0.97169 0 .0 0.4952o05? 1•33514F-02 1.4846 7 0.9760S 0.96854 0 .0 0.49526053 1.29004E-02 1.4848 7 0.97911 0.96834 0 .0 0.49526054 1.24712E-C2 1.48487 C .9/920 0.96717 0.0 0.4952o055 1 • 2052 5E-02 1.48407 0.97848 0.96658 0 .0
4 .2 1 609E-01 EXTRAPOLATION h IT H 35.4026 0.49526056 -7 .06613E-03 1.00000 - r - 59334 -0 .66495 0 .0 0.4952oG57 -9 .«5 2 7 8 F -0 3 1.484U7 1.39857 2.48084 0 . 0 0.49526058 -9 .39363E-03 1.41,487 0.93443 0.97067 0 .0 0.49526059 -8.84581E-0-* 1.48487 0.93284 0.97135 0 .0 0.4952606* 1.48487 0.91824 0.97165 0 .0 0 « 44526061 7.96604F-03 1.48487 -0 . 96408 -0 .96382 0 .0 0.49526062 7.71999E-03 1. 48 4 b 7 0.97683 0.92187 0 .0 0.49526063 7.53C2IF-C3 1.48487 C .98295 0.92493 0 .0 0.49526064 T.29847E-03 1.48487 0.97032 0.91606 0 .0 0.49326065 7.07626F-0'* 1.48487 0.97663 0.91333 0 .0 0.49526066 ' 67a3594E-0 3 1.45487 ■<j;$7267‘ 0 .93168 c . o 0 .49526067 6.59275E-03 1.48487 0.97102 0.96542 0 .0 0.49526068 6.37341E-03 1.48487 0.97310 0 956 45 0 .0 0.49526069 6 . 14o43E-03 1.4848 7 0.97C53 0 .95 7C3 c . o 0.49526070 ‘ ' 57906116-03 1. 4b 48 7 0.96 681 0.95514 u .u 0 . ‘t9?26071 5.67818E-03 1.48487 0.96/09 0.95465 o . c 0.49526072 5.454066-03 l.4 J 4 ff? 0.96598 0.95536 (i . 0 r49526073 5.24330F-03 1.48487 0 .966o0 0.95544 0 .0 0.49526074 5.03254F-0* 1.48407 0.96484 0.93217 0 .0 0.49526075 4.83131F-0? 1.48487 0.9648 5 0 .95 694 0 .0 0.49526076 ■ '477r6S7£H 5T 1.48487 C .98103 0.95377 0 .0 0.49526077 4.59862F-03 1.40487 0.97953 0 .9 5 3 n.t 0 .0 0.495260
" '7 5 ' 4.4765>5f:-d3 1.4846 7 0.97793 0.95403 0 .0 0.49526079 4.3525 7E-03 1.48487 0.97666 0.95243 o . c 0 . -,952606b 4.223826-03 1.48487 0. 9 )464 0.95372 0 .0 0.4952oU81 4.09508E-03 1.48487 0.9/361 0.95219 0 .0 0 49526082 3.96538E-03 1.48487 0.9/229 0 . 95C69 o . c 0.49526083 3.83S68E-03 L.484B 7 0.97113 J .951=1 0 . 0 (J.4 95 26084 5.706<53F-{)i 1.48461} ' 5.T7UI4 Jr5£vj32 t).0 1 0.49526085 3.57819E-03 1.48487 0.96885 0.95CC8 0 .0 0.49526086 3.4503 9E-03 1.48487 0.96 7 .*4 0.95046 0 .0 0.^9520087 3.32355E-0'1 1.48487 0.96056 0 .94LE I 0 .0 0.49526088 3 ,?0053 f-03 1.48487 0. $6!>ia 0. 94fc/5 0 .0 0.49^26089 3.07751F-0 ^ l.4 e *0 7 0.96464 0.94833 0 .0 0 . l9 3 C O 090 ' ~ ~y.'>J 5 7 3 V - D 7 ' " i ; ’4 ft767“ 0. 9&13T” 0 .946 3+ 0 .0 0 .49526091 ?.8410OF-a3 1.48487 0.9635U 0*95b24 0 .0 U . 49526097 2. 7256(5^-03 I . 484$? P .Q h Ji 1 0.961 45" c .o 0 .49526U93 2.6149 7E-03 1.48487 0.96203 0.96192 0 .0
' 6 . ’5 9 § 4 0 F -6 2 c XTRAPDLA i IuN WITH 25.2989 0.495*26094 1.4286UE-03 l .O C C C '1' C. 54775 0.48371 0 .0 0.495260
" W 1 . 48 4b 7 1.3^852 l . i & i l 88 0 .0 0 . t v j i b d9o 1.88160E-03 1.48407 0.94500 0 . 95 £29 0 .0 0.49526097 1•7652 5E-03 1.48487 0.93593 0 .$ 4 ? !7 0 .0 0.49526098 1 .6 4 3 1 8 E -0 3 1 .4 8 4 8 7 0 .9 3 2 4 9 0 .9? 282 o . c 0 .4 9 5 2 6 0$9 T .3 5 7 3 5 £ -o 5 1 .4 8 4 6 ? 0 .9 4 9 3 2 0 . $ 4 l C 0 0 .0 0 .4 9 5 2 6 0
100 1 .4 4 1 0 0 E -0 3 1.48487 0.9 2 6 7 3 0 .9 2 5 9 1 0 . 0 0 .4 9 5 2 6 0
END OF A D JO IN T CALCULATION - ITE R A T IO N TIME 0 .6 2 2 VINUTES
***** *****WARNING - FLUX CALCULATION NOT CCNVERbED**********0
I—1 O n H
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G Th c . » £ SQUARES CF T h e *ESltWt:> - ?i tL AJ I Vfc Ati SORPTION 0 » 9 j m i J K 1 h
GROSS NEUTRON BALANCE
GRP L FT LEAKAGE TOP LEAKAGE R1T LEAKAGE HOT LEAKAGE FNT l e a k a g e BAK LEAKAGE ri**2 LOSSES 1/V LOSS SPNCN LOSS1 - I . 4 7 4 4 6 S 6$2 -4 . 2 7 8 3 3 F 08
0 .00 .0
1.47446E 4.27B33E
09Ob
1 .6 4 3 8 6 E 13 5 .9 7 9 3 5 E 12
0 . 00 .0
Z . U O S ' . E l . 6 7t>75E
1212
0 . 0 0 . 0 O .C 0 . 0
0 .0 . C
3 - 2 . 3 5 5 9 1 E 084 - 1 .2 6 8 S 7 E 09
0 .00 . 0
2.35591E1.26857E
0809
2*975046 12 1 .6 9 5 5 7 E 13
0 .0o .o
9 . l 0 i 3 9 e0 .4 7 7 9 4 E
1112
O .C 0 .0 0 . 0 0 . 0
c .cc . o
SUM -3 . 4 0 6 4 6 E 09 0 .0 3 .4 0 6 4 6E 09 4 .2 3 4 8 75 13 0 .0 1.12035E 13 O .C O.C 0 .0
GRP AOSOBPT tONS 1 5 .202436 12
OU)r -S C A T T tR 1 .14969E 14
' SOUKCE 1.38706E 14
IN -S C A T1 E R 0 .0
TOTAL LCS5F.S 1.3H741E IS
TOTAL GAINS 1.3U/06E 14
PRCO/Ac SCk .p3 .6 5 6 1 S t -0 1
2 1 .2 3 787E 133 8 .5 0 2 5 4 E 12
9."494 256 13 8 .2 6 7 5 2 E 13
0 .6O .C
1 .1 4 9 6 9 6 14 9 .5 0 7 3 4 E 13
1 .1 4 9 7 7E 1-. 9 . 5 0 7 10b 13
1,1*969E9.5 0 7 3 4 E
1413
4 .0 0 1 4 6 E -0 1 3 i5 5 0 d 9 E —01
4 5 .907026 13 1 .3 0 8 i9 E 11 0 . 0 8 . * 6 ? s i t l i 8 .2 6 3 4 ? E 13 B.2C/51E 13 S. V S 76I t - 0 1
SUM B . 515395 13 2 .9 2 7 1 8 E 14 1.3B706E 14 2 .9 2 7 1 8 E 14 4.3 1 4 2 4 E 14 4.31424E 14
A gm c c PLOyg T BV ?nTiE-5Rff"CRnUP
ZONE 1— COITE 20NE 1 2 .2 2 7 1 7 E 11 7.27708E 1C 3 . 5 2 5 a : t 1C 1 .8 8 6 0 9 E 11
£ONE 2— CORE ZONE 29 . ‘ 3 4 0 & 10 6 .3 0 7 4 2 E 10 3.348<>4E 10 2 .2 8 7 7 7 E 11
TORE ' 3 — AXIAL" ^ D T T T 0 . 0 0 . 0 0 .0 0 . 0
IONE AVERAGE POWER DENS I T lE S t W A T T S / C C >6 .8 9 3 3 4 E 02 0 . 0 0 . 0
THE MAXIMUM PUUEK DcNSl l Y I H A M S / C L l A l KUW ANU LULUMN 4 AND L IN E 16 IS / .5947C5E 02
T h e s u f f e r9 .9 9 9 9 9 6 F -
paher d e n s i t y•01 9 .9 9 9 4 4 3 E -
ALONG ROW 9 I S 01 9 .9 9 9 8 6 2 E —01
7.5941676 02 AND THE RELATIVE PUwEK O E N S IT I ESIFRACT ION OF AVERAGE) 1 .0 0 0 0 M E 00
ARE
THE AVERAGE POWEH D ENSITY DOWN COLUMN 4 IS 7 . 349053E C2 AND THE RELATIVE POWER D E N S IT IE S ARE8 .$ 9 0 4 2 2 E - 1 .0 3 0 9 3 IF
01 8 .8 0 4 0 1 5 E - 00 1 .0 2 4 7 8 BE
61 9 .0 1 1 3 6 9 C -0 1 00 1 .0 1 6 0 4 3E 00
4 .2 ll6>& E -01 9.609258E—01 9.99B122E-01 1.0203t»oS 00 1.005644E 00
1.030815E 00 1.033426E 00
THE AVERAGE POWER DENSITY ALO^G LINE 16 IS 7.078665E 02 AND ThE RELATIVE POWER DENSITIES ARE1.008415E 00 I ,006801E 9 .735064E-0I 9.778190E-
00 1.003693E 0001 9 . 879075E-01
9.99290ZE-01 9.939139E-01 9.BB0U59E-01 9.B21723E-01 1.00428&E 00 1.024763E 00 1.046901E Ou 1.072900E 00
9.7718 72fc—01 0 . 0
9 . 73S724E—01 0 . 0
T H E T A - R -Z CASE W ITH BLACK ABSORBER. PERIODIC____________________________________4X13X20X4 GROUP. 4160 POINTS STREAM OF C I T A T I O N CASES URML 72
PERTURBATION RESULTS------- D E L T A -K / (K * D E L T A - S ) WHERE S REPRESENTS MACRO. CROSS S E C TIO N S . LAM BDA(PHI* M P H I ) = 1 .1 5 0 6 7 9 E -0 5
COMP NAME GRP S IG A ,S IG H ,0 B * * 2 NU*SIGF O I F F . COEF. B**21 CORE ZONE 1 1 - 1 . 5 9 3 9 1 OE 02 3 .2 1 8 3 0 3 E 02 -9 .1 6 4 7 8 0 E - 0 3 -2 .8 5 4 7 8 5 E 02
2 -6 .3 1 3 2 6 0 E 01 1 .C 4 8 6 4 8 E 02 —9 .1 7 1 3 7 0 E—03 -8 . 9 6 4 2 5 6 E 013 - 3 . 5 6 6 5 3 6E 01 5‘. 0761 76 E 01 — 7 .5 1 6 1 7 2 E —03 — 5 . 116479E 014 - 2 . 1 2 4 0 3 7E 02 2 .7 0 6 6 0 9 E 02 —3 .9 7 8 2 3 5 E — 02 -2 .U 8 0 9 7 9 E 02
2 CORE ZONE 2 1 -1 .7 9 7 3 9 8 E 01 3 .6 2 9 1 7 5 E 01 - 5 . 3 0 5 7 7 5 E -0 3 -1 . 8 5 8 3 2 6 E 012 — 1. 329042E 01 2 .3 9 5 8 7 1 E 01 — 1 .6 8 3 3 7 3 E — 03 — 1 . 174343E 013 - 7 . 6 4 7 3 1 5E 00 1 .2 7 1 4 8 7 E 01 - 6 . 7 9 5 2 7 6 E - 0 4 - 6 . 794799E 004 -5 .4 $ 8 5 3 4 E 01 d . 6 8 3 0 7 6 E 01 4 .9 4 2 4 5 4 E - 0 3 — 4 . 542433E 01
3 AXIAL BLKT 1 1 0 .0 0 . 0 0 . 0 0 .0I 6 .5 " 0 . 0 U .O 0 .03 0 . 0 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 0 . 0 0 . 0
TOHP-----------NOTE-----------K " SKibH-UUH ALL i m . KKT tTCTP . TCI-------------------------------------------1 CORE ZONE 1 1 1 .5 9 3 9 1 OE 02 5 .1 9 3 5 7 3 E 01 2 .5 1 4 0 4 6 E C l 1 .3 4 0 4 8 5 E 02
2 1 .9 4 1 7 4 3 E 02 6 .3 1 3 2 6 0 E 01 3 .0 5 4 707E 01 1.624093E 023 2 .2 7 1 4 9 7 E 02 7 .3 7 3 9 7 3 E 01 3 .5 6 6 5 3 6 E 01 1 .8 9 2 6 4 1 E’ 025 2 . 55/»U22F 02 S.2& 4315E O l 4 .0 O 5 9 3 7 E 01 2 .1 2 4 0 3 7 6 02
2 CORE ZONE 2 1 1 .79 7 3 9 8 E 01 1 .1 8 6 5 8 8 E 01 6 .2 9 7 2 1 4 E 00 4 .3 0 0 4 1 4 E 01----------------------------------------------------2 Z :0 iy n 6 E 01— i : 3 230*21 01— r.052'*22E' 00 ' l . t t l S U 'JE 01____________________________ 3 2 . I 8 6 7 9 1 E 01 1 .4 4 1 4 6 4 E 01 7 .6 4 7 3 1 5 E 00 S .2 1 9 7 8 9 E 01
4 2 . 2 70660E 01 1 .4 9 2 0 1 7 E 01 7 .9 1 2 6 3 6 F 00 5 .3 9 8 5 3 4 E 013 AXI AL BLKT 1 1 0 . 0 ______________OjO________________( K 0 _______________0 ^
2 0 .0 0 .0 ' 0 .0 0 .03 0 . 0 0 . 0 0 . 0 0 . 05 070 070 070 STo
END OF CASE - TOTAL CPU TIME WAS 1.56 MINUTES TOTAL CLOtK TIME WAS 7.12 MINUTES
* ********************************+***********************+** 4*******
* * * * * * * * * I H i s JOB HAS RUN ON 0 3 - 1 1 -V 2 GN THE IBM 3 6 0 / 91*********
TRIAGONAL 3 -D tT IG V * C A S E . t iN E -S IX T H WITH BLACK ABSORBER >__________________BX4X4X6 GROUP» 768 POINTS , STREAM UF C I T A T I O N CASES ORNL 72
' g e n e r a L T o n i ' r o I I n p u t - s e c t i o n 001
C Q O O O O O O O O O I O O O O O O I O O O O OI O O O I 0 0 0 I 0 0 I l O O O O O O O Q O O Q
Too 1 0 0 1 0 2 3 0 0 (J 0 0 0 0 0 0 0 0 0 0 12 6 12 6 12 2 4l.SPQftPOF f'O 5 .0 0 0 0 0 0 1 - C l 9 .9 9 9 9 9 9 F 09 9 .999S S 9E 23 0 . 0 _______________ l.OOOOOOE 00_________________
NEUTRON FLUX PROBLFM CESCRIPTI1IN - SEC TIGN 003
_ 2 _ 2 0 0 14 C____ 0____ C____ O P 0 0 1 1 0 1 3 0 0 0 0 0 0 09 . 9 9 9 9 9 9 E -0 5 1 .0 0 0 C O O F -0 5 9 .9 9 9 9 9 9 E - 0 5 9 .9 9 9 9 9 9 E - 0 5 9 .9 9 9 9 9 9 E -0 5 0 .04 .6 9 0 0 0 0 E -0 1 4 .6 9 0 0 0 0 F -0 1 1 . 016190E 03 1.OOOCCOE 00 1.6 6 f c 6 o 6 E -0 I 0 . 0 ____________________________
L F F I , TO P>? I G H T t BOTTOM >FRCNT , i ACK BOUNDARY CCNOITICr>S ARt___________________________4 .6 9 0 0 0 0 E -0 1 4 .6 9 0 0 0 0 E -0 1 0 . 0 0 . 0 4 .6 9 0 0 0 0 E - 0 1 0 . 0
rtOft PNt). Ct'NSfANt POR ALL GROUPS IN 2 Cn £ 3 T§ 4 .6 9 G 0 0 0 E -0 1
~ f H « E E HImTnS l a N A t ' t R I ANGULAR I » WIDTH 6 .1 2 0 1 7 2 b 01 HEIGHT 4 .S 9 C 1 3 8 E 01 DEPTH 6 .0 5 0 0 9 8 E 01
------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------Ha \
" r e C I PET •SPE CI F I CAT I ONS----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- ^PTS RFGION WIDTH_______________________________________________________________________________________________________________________________
8 5 .3 0 0 2 4 0 F 01 '
PT5 Rfc6(0N HEIGHT _______ 4 5 .3 0 0 2 4 0 E 01
PTS RFGION DEPTH3 3.OO0O99F Oi 1 3 .0 4 2 0 0 0 E 01
TT-f>lR. ' POINTS------ S-------------------- FTJITTrTO I NTS-------------------------------------------------------------- 5----------- Z-Bl'A. POINTS-4-----------------------------
u r sn n c c s t ct m e s h i m tl; k v a c i m e r f &c e s -------------------------------------------------------------------------------------------------------------------------------------------------------------------------
— 3— dtst;----------------------------------------------------------------------------------------------------------------------------------------------------2 7 .6 5 0 3 1 5 .3 0 0 4 22.951 5 3 0 .6 0 1 fe 3 8 .2 5 1 7 4 b . 901 8 S 3 .5 5 2 9 6 1 .2 0 2
1 n j S T .------ 2— rr.7 T5 ------------------------------------------------------------------3" 22.551------4" 3<r;426----------5" 457^ Cl -----------------------------------------------------
— (tr— c n m ~ --------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------2 1 0 .0 2 7 3 2r . 054 4 30.061 5 6 0 .5 0 1
01 STANCES T n PI.UX PO IN TS
j p i s t .T 57515 ? T T 7 4 7 5 3 1 9 .1 2 6 4 2 6 . 7 7 6 5 3 4 .4 2 6 6 427076 7 4 9 .7 2 6 B 5 7 .3 7 7
T-------ftftfi J WCM J ------------------------------------------------------------------------------------------------------------------------------------------------------------------1 3 .8 2 5 . 7 .6 5 C 2 1 5 . 3 0 r 1 9 .1 2 6 3 2 6 .7 7 6 3 C .6 0 1 4 3 8 .2 S 1 4 2 .0 7 6
k b n i « T 1 5 .0 1 3 2 15.040 3 25.067 4 45.251
iO N F INPUT BY 1RFGION
PLANE NUMBER ?
1
PLANE NUMBER 22
{ONE NUMBER AT EACH MESH INTERVAL
$ p £ £ IM £ A Y f t iN M ft l a y e r n u m b e r i
1 2 3 4 5 6 7 8
1 2 2 2 2 2 2 2
2 2 2 2 2 2 2 2 2 2
" T ...... J - ' J T T4 2 2 2
J 2 2 2 2 2 2 2 2 2
S P E C I F I C A T I O N f o r LAYER NUMBER 2
____1___ 2___3__ 4 S 6 7 8
1 2 2 2 2 2__ 2 2___2I ? 2 ? 2 2 2 “ I 23 2 2 2 2 2 2 2 2■5— r r T T T T t - r
T P F C r F l C Z T r O N F O R 'IA Y ? K NDHOE'IT"" 3
I 2 3 4 ' b 6 7“ # " ......................
1 2 2 2 2 2 2 2 27. 2 2 2 2 2 2 9 2* 2 $ 4. £ 2 2 i 24 ? 2 *> 2 2 2 2 2
S P E C IF IC A T IO N f o r LAYEP NUMBfcR 4
1 2 J 4 5 b 7 8
1 2 2 2 2 2 2 2 22 2 2 2 2 2 2 2 23 2 2 2 2 2 2 2 24 2 2 2 2 2 2 J 2
MPSH OVERLAY INPUT
20*iff"KuMB,£u 31 7 1 1 1 4 1 ■» 2 2 1 4 1 2 3 3 1 4 1 1 4 4 1 4
2 ONE NUMBFR 1
6 8 3 * 1 3 5 5 4 4 1 3
ZONE NUMBER AT EACH MESH INTERVAL
& P fc C IF IC it lO N FOR LAYff< NUMBER T
1 2 3 4 5 6 7 6
12
3 3 3 3 3 3 3 2 3 3 3 2 2 2 2 2
"5 3 2 2 2 T i l l___i i
34 3 2 2 2 1
S P E C IF IC A T IO N FOR LAVER NUMBER 2
1 2 3 4 6 6 7 8
3 3 3 3 3 3 3 22 3 3 3 2 2 2 2 23 3 3 2 2 2 1 1 1
“S 5 2 2 T r n ’T
“S p f c d lf lC A T lO N fOR LAV^ft tjUMfllR T
--------------------r r * " 5 ' T 5"
1 3 3 3 3 3 3 3 22 3 3 3 2 2 2 2 2i— 5 '3' * 2 1 V I4_____ 3 2 2 2 1 1 1 1
HONCT\
S P E C IF IC A T IO N FOR LAYER NUMBER 4
1 2 3 4 5 6 7 8
3 3 3 3 3 23 3 3 2 2 2 2 23 3 2 2 2 2 2 2
1 2 2 2 2 2 2 F
> ! S S t O N SOURCE D IS T R IB U T IO N AND SUM 0 .7 5 6 0 0 0 .2 3 4 0 0 C.OIOOO oTo" 0 . 0 0 . 0 1.000i>0
CORfe stOftAftf t ) lF^EftlNCe (wGM>si e6UaTtbKi tflNSTAtiiTS T70 lT i i t e A b " 5 P " s f a R E D 2 i 2u'
f t y j A f i M CflWStANTS WILL ftE STOftEO I N CORE- ' " " “ .............................................. ............
NUMfft — c o l u m n s , AflwS, H a n e s , g r o l ,j5 . u K C A T , NT*TKs c a T , RfjH oN S ,' a n d z o N ts 8 4 4 6 0 2 S 3
N E W Y LO C A TIO N 5 R6 5FRVED FOP DATA STuHACt— 4 0 ( 0 0MEMORY LOCATIONS USED F09 T H I S PROBLEM----------- 7312
,W Jm o r v l Oc A T I o ^ s B U T U 5 T 0 -------------- -------- - - - — ; " 326eB 1 ■ ■ ....... ■ ■ ■
BX4X4X6 GROUP* 7 « POINTS STREAM OF CITA TIO N CASES ORNL 72L I N E RELAXATION W ILL BE OCNE CM RflwS - 3 INNER M E K A T iU N t S tITERATIO N f l u x c h a n g e 06tfi MU-1 M U -2 MU-3 K
I 3 .5 0 3 6 2 = 0 0 1.0 0 0 0 0 7.0 0 7 2 4 - 1 . 9 9 1 2 5 0 . 0 0 . 5153dd2 - 9 . 0 7 0 4 8 E - 0 1 1.76171 - 1 . 1 6 5 9 4 - 0 . 0 0 3 3 4 0 .1 5 3 1 7 0 .5 9 7 6 4 13 6 .3 7 3 2 5 E -0 1 1.6 1 5 1 2 - 0 . 0 6 5 3 1 - 1 . 2 5 3 2 4 0 .9 8 4 0 3 0 .6 6 3 1 8 04 - 4 . 8 6 2 9 6 6 - 0 1 1 .5 3 6 4 9 - 1 . 2 4 9 3 2 - 0 . 2 4 4 4 8 0 .6 0 4 7 5 0 .6 9 8 9 6 45 - 3 .5 7 2 8 4 E -P 1 1 .4 9 7 ? 7 0 .3 7 742 0 .3 7 5 5 3 0 .4 6 6 3 1 0 .7 1 5 2 5 16 - 2 .6 4 B 9 1 F -0 1 1 .4 7 8 6 * ' o . 3 f h i 0 .4 8 5 5 1 0 .4 3 2 3 8 0 .7 2 2 2 6 07 -9 . 9 4 8 7 9 E - 0 2 1.4 6 9 6 5 0 .3 7 4 5 1 0 .5 2 3 5 7 0 .4 1 8 1 7 0 .7 2 5 2 0 0a -4 . 6 7 5 4 9 E - 0 2 1 .4 6 5 7 6 0 . 36889 G . 50361 0 .4 1 3 1 9 0 .7 2 6 4 2 79 - 1 . 6 0 6 0 8 E - 0 2 1.4 6 3 8 6 0 .3 7 8 0 2 0 .4 8 6 4 9 0 .4 0 7 2 7 0 .7 2 6 9 3 /
10 - 6 . 4 9 2 6 7 F - 0 3 1.4 6 2 9 8 0 .3 9 7 7 6 0 .5 0 4 8 0 0 .3 9 9 2 4 n .7271461! -2 . 5 8 8 9 3 E - 0 3 1 .4 6 2 5 7 0 .3 9 6 1 6 0 .5 3 7 7 1 0 .3 8 4 0 4 0 .7 2 7 2 3 1
1.46<>*a 0 . $9461 0 . 5 ^ 4 4 9 0 .3 5 1 2 6 0 .7 2 / 2 o 413 - 4 . 0 2 9 8 7 E -0 4 1 .4 6 2 3 0 0 .3 9 2 8 4 0 .5 0 7 7 9 0 .2 8 1 9 7
-3 . 2 9 6 9 4 E - 0 4 EXTRAPOLATION WITH 0 .8 1 9 2 0 .7 2 7 2 8 914 5 .6 2 6 6 8 E -0 S l .O T C / 'n - 0 . 1 3 9 5 7 - 0 . 1 2 4 4 9 0 .1 4 3 0 1 0 .7 2 7 2 U 615 - 1 . 6 8 6 8 1 E - 0 5 1.4 6 2 2 4 - 0 . 2 9 9 8 0 - 0 . 3 5 4 49 - 4 . 5 4 1 1 9 0 .7 2 7 2 8 616 - 1 . 2 1 5 9 3 F - 0 5 1.4 6 2 2 3 0 .7 2 0 8 4 0 .0 6 6 6 7 1 .0 0 4 9 9 0 .7 2 7 2 8 6
END O F EIGENVALUE CALCULATION - IT E R A T IO N T I K E 0 .C 4 6 MINUTES
CONVERGENCE IN D IC A TIO N RY M IN IM IZ IN G THE SUM OF TH E SQUARES OF THE RESIDUES - R E L A T IV E ABSORPTION 0 .9 9 9 9 9 7 0 K 0 .7 2 7 2 8 2 8
L E A K A G E 8 .0 9 2 2 6 E 05 TOTAL LOSSES 3 .2 5 5 0 1 E 06 TO TAL PRODUCTIONS 2 .3 6 7 3 3 E Ob REACTOR POWERtWATTS) 1 .0 1 6 1 9 E 09
A 0 J0 1 N T PROBLEM FOLLOWSIT E R A T IO N FLUX CHANGE BETA MU-1 M U -2 MU-3 K
1 1.37494E 30 1.00000********** - 0 . 5 6 6 7 8 0 . 0 0 .7 2 7 2 8 62 2.S 4 5 0 0 E 00 1.76171 2 .6 4 5 0 G 0 . 2 5 8 5 8 0 . 0 0 .7 2 7 2 8 63 6 .8 1 2 8 6 E -0 1 1.6 1 5 1 2 0 .9 2 0 7 5 0 .7 0 7 3 2 0 . 0 0 .7 2 7 2 8 64 2 .4 0 3 1 8 E -0 1 1 .4 3 6 4 4 b . i l i 4 s 0 .2 ^ 6 2 8 5.(J 0 .7 2 7 2 d 65 1 .0 4 8 6 0 E - 0 I 1 .4 9 7 3 7 0 . 46605 0 .5 8 9 0 5 0 .0 0 .7 2 7 2 8 66 5 .9 1 0 0 2 E -0 2 1 .4 7 8 6 5 0.6 2 2 7 1 0 .5 7 0 2 9 0 . 0 0 .7 2 7 2 6 67 2 . 5 8 9 9 9 E - 0 2 1 .4 6 9 3 5 0 .4 6 4 1 4 0 .3 3 2 7 5 0 . 0 0 .7 2 7 2 8 66 1 .0 5 2 0 P E -0 2 1 . 4 ( 5 7 6 0 .4 1 6 7 0 0 .4 7 8 4 0 0 . 0 0 .7 2 / 2 8 69 4 .4 6 5 1 0 E -P 3 1 .4 6 3 8 6 C . 42891 0 . 4 7 3 8 0 0 . 0 0 .7 2 7 2 8 6
‘ " I f f " 1 .4 6 3 6 ^ 1 -0 3 1 .4 6 2 9 8 d . 4 4 l 7 J 0 .4 1 6 8 8 6 . 61 .6 7 1 5 2 E -0 3 EXTRAPOLATION WITH 0 .8 5 2 9 0 .7 2 7 2 8 6
11 -•9.787<'8E-05 I k 00000 - 0 . 0 4 9 9 4 - 0 . 1 2 1 5 0 c . c 0 .7 2 7 2 8 612 - 2 . 7 8 9 5 0 E - 0 5 1 .4 6 2 3 8 0 .2 8 4 9 9 0 .2 1 8 7 6 0 . 0 0 .7 2 7 2 8 613 - 1 . 7 5 2 3 8 E-0 5 1 .4 6 2 3 0 0 .6 2 8 1 9 0 . 0 0 . 0 0 .7 2 7 2 8 b
SMB O f A D JO IN T CALCULATION - IT E R A T IO N TIME 0 . 0 2 7 MINUTES
CONVERGENCE IN D IC A TIO N RY M IN IM IZ IN G THE SUM OF THE SQUARES (if THE RESICUES - R E L A T IV E ABSORPTION 0 .9 9 9 9 9 1 8 K 0 .7 2 7 2 4 1 5
GROSS NEUTRON .BALANCE
GRP L F T LEAKAGE TOP LEAKAGE H I T LEAKAGE BOT LEAKAGE FNT LEAKAGE b a k l e a k a g e B**2 LOSSES 1/V LOSS XtNUN LOSS1 0 . 0 0 .0 0 . 0 0 .0 2 .4 8 7 0 9 E 05 0 .0 0 . 0 0 . 0 0 . 02 0 . 0 0 . 0 4 . 0 0 .0 3 .4 2 1 6 0 E 05 c . o O .C 0 . 0 0 .03 0 . 0 0 . 0 0 . 0 0 . 0 1 .6 0 1 2 1 E 05 0 . 0 0 . 0 0 . 0 0 . 04 n . n A .o O .C 0 . 0 4 .2 4 2 1 4 E 04 0 . 0 0 . 0 0 . 0 O.U5 0 . 0 0 .0 0 . 0 0 .0 1 .4 6 7 5 0 E 04 0 . 0 0 . 0 0 . 0 0 . 06 0 . 0 0 .0 0 .0 0 .0 1.14016E 03 0 .0 0 .0 0 . 0 0 .0
SUM 0 . 0 o . r 0 . 0 0 .0 8 .0 9 2 2 6 E 05 C .O 0 . 0 0 . 0 0 . 0
GRP ABSORPTIONS O U T-S C A TTE R SOURCE 1N -S C A TTE R TO TA L LOSSES TGTAL GAINS PROD/ABSCKP12
4 .2 1 5 7 5 E 05 6 .7 0 9 2 1 E Ob
I .7 9 0 5 2F 1 .4 4 6 5 7 F
0606
2.46078E7.61671E
0605
0 .01 .6 9 7 9 8 E 06
2 .4 6 0 8 0 E2 .4 5 9 6 4 E
0606
2 .4 6 0 7 8 E Oo 2 .4 5 9 6 5 E 06
2 .2 8 3 1 1 E 00 9 .8 6 9 7 4 E —01
34
8 .05 7 6 0 E 05 3 .4 9 6 0 8 ? 05
6 .05491E2 .1 ? 7 3 B E
0505
3.25 5 0 0 Er . e
04 1 .5 3 8 8 2 E 06 6 .C 5 7 6 9 E 05
1 .5 7 1 3 7 E6 .0 5 7 6 7 E
0605
1.57138E 06 6 .0 5 7 o 9 E 05
5 .3 8 3 1 4 E -0 14 .9 4 4 2 2 E - 0 1
56
1.6672*E 05 3 .1 1 9 8 4 F 04
3 .2 3 3 8 0 E0 .0
04 0 . 00 . 0
2 .1 3 7 3 8 E 05 3 .2 3 3 8 6 E 04
2 .1 3 7 3 8 E3 .2 3 3 8 6 E
0504
2 .1 3 7 3 8 E 05 3 .2 3 3 8 b E 04
6 .6 6 7 8 0 E -0 17 .S 7 0 2 9 E -0 1
SUM 2 .4 4 5 7 8 F 06 4 .0 B 8 64 E 06 3.2 5 5 0 0 E 06 4 .0 8 8 6 5 E 06 7 .3 4 3 6 6 E 06 7 .3 4 3 6 5 E 06
AVFRAGE FLUXFS BY 70NF AND GROUP .
ZONE 1— CORE ZONE 12 . 415615 03 4 . 05780E 03 2 . 31776E 03 7 .5 5 8 1 5 E 02 2 •60457E O i! 1 . 73443E 01
ZONE1.
2— CORE ZONE 2 74447E 02 6 .9 2 0 5 5 6 02 5. 67905E 02 1 .7 9 8 7 1 E 02 5 . 2 8 6 16E 01 6 .6 36C7E 00
ZONE 3— AXIAL BLKT 10 . 0 0 . 0 0 . 0 0 . 0 0 . 0 0 . 0
ZONE AVFPAGE POWFR DENS ItIESIrtATT S/CC) B.51647F 03 4.62631E 02 OrO
THE MAXIMUM POWER DENSITY( WATTS/CC) AT ROW 4 ANC COLUMN 8 AND LINE 3 IS 1.426184E 04
THE AVERAGE POWER OENSITY ALONG ROW 4 IS 7.052707E 03 AMD THE RELATIVE POWER DENSITIES!FRACTION OF AVERAGE! AREO 4.04^2636-02 nT56428E-01 2.825584E-01 1.177644E 00 1.572985E 00 1.79062CE 00 2.02218GE 00
THE AVERAGE POWER DENSITY DOWN COLUMN 8 IS 6.908465E 03 ANC THE RELATIVE POWER DENSITIES ARE4.131749F-02 2.884 573E-01 1.605826E 00 2.0644C1E 00____________________________________________________________________________________
THE AVERAGE POWER DENSITY ALONG LINE 3 IS 6.258816E 03 AND THE RELATIVE POWER DENSITIES ARE 1.190118*: OC 2.1194516 OC 2 .2 73680E OC 1.468655E-01
TRIAGONAL 3-D (T1GAR CA SE. ONE-SIXTH WITH BLACK ABSORBER)8X4XAX6 GROUP, 768 p r i M s STREAM OF CITATION CASES ORNL 72
PER TUR RAT ION RESULTS— -Dfc L TA -W ( K*JEL tA -S ) WHERE S REPRESENTS MACRC. CROSS SECTIONS. LAMBOA(PHI* N P H I» = 5.2931OOE—21
COMP NAME GRP SIGAtSIGR , DB**2 NU+SIfcF OIFF. COEF. B**21 CORF ZONE 1 1 -1 .3 8 0 7 5 1 ? 01 1 .8 5 5 6 5 6 E 01 - 3 . 6 6 8 6 1 3 E - 0 2 -3.69/7S7E 01
2 -2.092856E 01 3 .108162E 01 —6 . 182/55fc-02 —3 .346297E 01? -1.267972E 01 1.772644E 01 —3 . 85/o75E-02 -1.480748E 014 -4.454264£ 00 5.80146QE 00 -• 1 .5K »ti20e-C2 —4.099686E 005 -1 .748740E 00 2.007670E 00 -6 .115556E-03 -1.747541E 006 -1 .49754 3F-01 I • 332244E--01 —4 . 595984E—04 —1 .4 52140E-01
2 CORE ZONE ? 1 - 1 . 3 9 4 ‘»5?r 0? 1 .7 6 7 0 9 6 E 00 - 4 . 3 5 9 6 7 2 E - 0 2 -2 .4 7 6 9 9 5 E 002 -3 .3 6 5 0 3 8 E 00 6 . 336025E 00 - 7 . 0 1 5 6 2 2 E - 0 2 —3 .6 4 1 7 9 1 E 00a ~ 2 . 0 9 0 5 1 7E 00 4 .9 5 5 6 6 5 E 00 —4.146499E—02 -1 .5 7 7 5 0 1 E 004 -6 .1 3 l « J 6 5 f e -0 l 1 . 5 4 2 7 1 I E 00 - 1 .3 8 8 9 4 8 E -0 2 —4 .0 7 9 2 0 7 E -0 15 - 2 . 1 2 ! 24 3 E-01 4 .5 4 7 2 0 4 E --01 - 5 . 5 7 16B6E-03 —1 .5 6 0 3 0 1 E -0 16 - 3 . 0 3 0 2 4 2 E - 0 2 5 .4 5 9 6 d 2 E --02 —3 .6 5 5 5 9 5 E— 04 —2.4997 64E-02
3 AXIAL BLKT 1 1 0 .0 U.O U.O 0 .02 o . c 0 .0 0 .0 0 .03 0 .0 0 .0 0 .0 0 .04 6 .6 6 .6 U.O 0 .0 <5 0 .0 o . c C.O 0 .06 0 .0 0 .0 0 .0 0 .0
COMt> KFS7TE 6RPT'K ■ --- 51G5 (PROH"'AL'f'GRps. kk Vo 6 p p . k JI CORE ZONF 1 1 1« 3B0751E 01 2 .3 1 2 9 0 6 E 01 1 .3 1 9 1 6 5 E 01 4 .3 1 6 9 8 9 E 00 1 . ‘♦936026 00 9 .9 1 3 4 5 6 E -0 2
’ 2 1 .2 4 9 B4 4 E 01 2 .0 9 2 B 5 6 E 01 1 .1 9 3 3 8 5 E 01 3 .90 6 6 9 1 E 00 1 .3 5 2 4 0 9 E 00 8.971459E-02~____________________________ 3 I .3 2 8 4 3 6 F 01 2 . 223987E 01 1 .2 6 7 9 7 2 E 01 4 .1 5 1 4 7 6 E 00 1 .4 3 7 4 4 7 E OC 9 . 5 3 3 5 4 2 E - 0 2
4 1 .4 2 6 0 B0 E 01 2 .3 B 6 7 8 4 E 01 1 .3 6 C 4 4 7 E 01 4 .4 5 « 2 b 4 E 00 1 .5 4 2 4 4 5 E 00 1 .0 2 2 T 9 9 E -0 15 1 .6 1 7 0 2 4 E 01 2 .7 0 6 5 0 5 E 01 1 .5 4 2 7 1 4 E 01 5 .0 5 0 5 3 9 E 00 1 .74 8 7 4 0 E 00 1 .1 5 9 6 9 0 E -0 15 > .0 8 8 4 U 6 E o l 3 .49!>628t 01 l . $ 9 2 t > I § t <T1 6 .5 2 2 2 0 7 E 00 2 .2 5 7 S B 5 E 00 1 .4 9 7 5 4 3 E -0 1
_ 7 C0RE ?0NE 2 1 !»39<>!>5£E 00 5 .0 1 7 7 4 8 E 0 0 3 .9 3 2 0 7 4 E 00 1 .235026E 00 3 .6 1 0 6 8 8 E -0 1 4 .3 4 2 9 8 0 E -0 2~ 7. S.b"30U74E—01 3 . 3t>5038E 0 0 2 .6 0 9 5 5 2 k 00 8 .0 9 4 6 7 6 E -0 1 2 .3 B 6 3 7 4 E -0 1 2 .S 4 2 0 B 7 E -0 2
____________________________ 3 7 .8 8 1 5 5 4 E -0 1 2 .726971E 0 0 2 .0 9 0 5 1 7 E 00 6 .4 5 3 3 S 7 E -0 1 1 .9 0 2 8 4 4 E -C 1 2 .2 4 I 1 1 2 E -0 24 7 . 5 ? " 4 ? 4 E - C 1 2 .5 9 5 2 2 2 E 0 0 " 1 .9 6 / 0 7 5 E 00 6 . 1 31905E-01 1 .B 0 8 4 5 3 E -0 1 2 .1 2 7 3 6 8 E -0 2•> 8. 7 4 2 9 6 7 E-0 1 3 .0 3 1 5 7 0 E 0 0 2 .3 2 7 8 1 4 E 00 7 .1 9 2 4 6 6 E -0 1 2 .1 2 1 2 4 3 E -0 1 2 .5 0 2 3 9 6 E -0 25 l . '0 5 5 3 ? 6 E ffi) 3 .o 6 3 5 * 5 E 06 2 .B 1 5 2 $ 9 E 00 8 .7 0 2 0 3 0 E -0 1 2 .5 6 6 5 6 6 E -0 1 3 .0 3 0 2 4 2 E -0 2
3 AXIAL RLKT 1 1 C.O R.O 0 .0 O.C 0 .0 0 .05T 0 . 0 "570 57 5 0 .0 0 . 0 0 .03 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0_ ^ 57^ 5 7 c oTc c . o5 0 .0 0 .0 0 .0 0*0 0 .0 0 .0
------------------------------------ 5 B77J----------------- 073“ ----------------------373--------------------- 373-----------------------575----------------------oTo
THb U F " C IT P ~ T O m CPU TIME WAS-----KTITMIHUTB----- njTlfCnCLCCK tTMG '(Ws-----6.8i MINUTE'S'
TTC T T iiW W Tri l S 3nB' 6'JTS RUM AN— 0 3 -1 1 -7 ? — ON"THE "IBM SoCW l*********
TH E T A -R -Z CASF TO COMPARE TR1AGONAL. O N E-TH ELTH U T H BLACK ABSCRBEK 8X 15X 4X 6 GROUP, 2680 P O IN TS STREAM OF C I T A T I O N CASES ORNL 72
*5En £r a l c o n I r o l lN P u r " r _ T E T t T W o o i
0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 1 0 0 0 1 0I 0 0 0 I 0 0 0 1 0 0 1 1 0 0 0 0 0 0 0 0 0 0 0
2oo lo o 10 1 .5 0 0 0 0 0 E PO
2 3 0 * . OOOOOOE
0-0 1
0 0 0 9 .9 9 9 9 9 9 E 09
09 .
0 0 99S999E
023
00 .0
0 0 01
12 o .OOOOOOE
1200
6 12 24
NEUTRON FLUX PROBLEM DESC R IP TIO N - SEC TIO N 003
0 0 0 0 12 0 0 P 0 0 1 1 1 0 0 1 3 0 0 0 0 0 0 09 .9 9 9 9 9 9 E —05 1 .0 0 0 0 0 0 E -0 5 ♦ .6 9 0 0 0 0 E -0 1 4.690000C— 01
9 .9 9 9 9 9 9 E - 0 5 9 .9 9 9 9 S 9 E -0 5 1 . 0 1 6190F 03 1 .0 0 0 0 COE 00
9 .9 9 9 9 9 9 E —05 8 .3 3 3 3 3 1 E -Q 2
0 . 00 . 0
L E F T ,T O P ,R IG H T .B O T T O M .F R O N T ,B A C K BOUNDARY CCNDIT1CHS ARE0 . 0 0 . 0 0 . 0 4 .6 9 0 0 0 0 E -0 1 4 .6 9 0 0 0 0 E — 01 0 . 0
■ffOTTKND. CONSTA'KiT Pflft ALL' GftOuPS IN ZCNE— 3— T5— 5T39ofc0iie-o T
THREE DIMENSIONAL C Y LIN D R IC A L f lE O M F T K Y IR "T h CTT7li WIDTH 5 .2 3 5 9 9 7 ^ -0 1 HfcJGH7 5 . 737698E 01 DEPTH 6 .0 5 0 0 9 8 E C l
REGIONp r s
S M C IF IC A T If lN S REGION WIDTH
12
5 .2 4 0 0 0 0 E -0 21 .2 2 2 0 0 0 E -0 1
1 6 .2 7 9 9 9 9 E-0 2 1 5 . S 30000E-02 I O .S 7 9 9 9 6 E -0 2 1 8 . 8G9996E-02 1 6 .8 9 9 9 9 5 E -0 2
PTS REGION HEIGHT4 2.6^505? 61 4 7 . 9 2 4 9 9 66 J 1 .428100E 61 4 8.671U 00E 00
p t S3
RE6I0N bEPTH 3 .00B 099E 01 1 3 .0 4 2 0 0 OE 01
X - D I R . POINTS 8 V - D I R . POINTS 15 Z—D I R . POINTS 4
OISTANCES TO MESH INTERVAL INTERFACES
J D I S T .2 C .C 5 2 3 0 .1 1 5 4 0 .1 7 4 5 0 .2 4 4 6 0 .3 3 2 7 0 .4 0 1 8 0 .4 6 2 9 0 . 524
1 .u i s r .2 1 3 .2 5 0 3 1 8 .7 3 8 4 2 2 .9 5 0 5 2 6 .5 C 0 0 2 8 .6 8 7 7 3 C .7 1 9 8 3 2 .6 2 5 9 3 4 . 425 10 3 9 .7 5 9
11 4 4 .4 5 8 12 4 8 .7 0 6 13 51 .0 1 2 14 5 3 . 2 1 8 15 5 5 .3 3 7 16 5 7 .3 7 7
Kft DIST ? 1 0 .0 2 7 3 2 0 .0 6 4 4 30.081 5 6 0 .5 0 1
DISTANCES TO FLUX POINTS
J D I S T .1 0 .0 2 6 2 0*CB4 3 0.145 4 0 .2 C 9 5 P . 288 6 C .367 7 0 .432 8 G.493
D I S T .
10 4 2 .1 7 4 11 46 .631 12 49 .8 7 2 13 5 2 .1 2 7 14 5 4 ;2 8 8 15 i 6 . 3 6 6
KB D IS T 1 5 .0 1 3 2 15 • 040 3 2 5 .0 6 7 4 4 5 .2 5 1
•ZONE INPUT BY REGION
PLANE NUMBER 11 I I2 2 2
1 12 I
11
11
2 2 2 3 3 3
2 2 3 3
23
2a
PLANE NUMBER 22 2 i 2 2 2
2 2 2 2
£2
>2
2 2 2 3 3 3
2 2 3 3
23
22
2 ONE NUMBER AT EACH MESH INTERVAL
S P E C IF IC A T IO N FOR LAYER NUMBER I
1 2 3 4 5 6 7 8
1 1 1 1 1 1 1 I'2 1 1 1 1 1 1 1 1 '3 1 1 1 1 1 1 1 14 1 1 1 1 1 I 1 15 2 2 2 2 1 1 1 16 I 2 2 2 1 1 17 2 2 2 2 1 1 1 16 t 2 * 2 1 i 1 1 " "9 Z 2 2 2 2 2 2 2
to t t 2 2 t 2 211 2 2 2 2 2 Z 2 212 3 3 3 3 3 3 2 z13 3 3 3 3 3 3 2 214 " 3 3 3 3 3 3 2 215 3 3 ■? 3 3 3 2 2
SPECIFICATION FOR LAYER NUMBER 2
1 2 3 4 5 6 7 8
1 1 1 1 1 1 1 1 12 1 1 1 1 1 1 13 1 1 1 1 1 1 1 14 1 1 1 1 1 1 i 15 2 2 2 2 1 1 1 16 2 2 2 2 1 1 1 ' "? 2 2 2 2 1 1 1B 2 2 2 2 1 1 1 19 2 2 2 2 2 2 2 2
1ft 2 2 2 Z 2 2 2 211 2 2 2 2 2 2 2 212 3 3 3 3 3 3 2 Z13 3 3 3 3 3 3 2 ?
14 3 3 3 3 3 3 2 ?15 3 3 3 3 3 3 2 2
SPfr. ! F IC A T IO N FOR LAYER NUMBER 3
_ J _ . 2 3 4 5 6 8 __________ ___
l 1 I 1 1 1 1 1 1"2 1 1 1 1 I 1 1 13 1 i 1 1 1 1 1 14 1 i 1 1 1 1 1 1» 2 2 2 2 1 1 1 1b 2 ? 2 2 1 1 1 i7 2 7 2 2 1 1 1 18 2 2 2 2 1 1 1 19 2 2 7 7 2 7 2 2
I P " 2 2 2 2 2 2 2 21! 2 7 2 2 2 2 7 212 3 3 3 3 3 2 ?13 3 3 5 3 3 -a 2 214 3 3 3 3 3 3 7 ?15 3 ? ■» 3 3 3 2 ?
SPECIFICATION CQR LAYER NUHAF R 4
I 2 a 4 5 6 7 a
1 2 2 2 2 2 2 2 2"2 ' 2 2 2 ? 2 2 2 7
3 2 2 2 2 2 2 2 7T * i ? i 2 7 2 i 2
5 2 2 2 2 2 2 2 26 i 2 2 2 i 2 2 27 2 2 2 2 2 2 2 2e 2 2 2 2 2 2 2 29 ? 2 z 2 2 2 2 2
In 2 2 7 2 2 •> 2 311 2 2 2 2 7 2 2 2
'1?' 4 3 J 5 J 3 213 3 3 3 3 3 2 214 ‘ S 5 5 3 3 S t ?15 3 3 3 3 3 3 2 2
MESH o ver lay INPUT
ZONE NUMBER 12 4 s 5 1 3 4 4 6 6 1 3
ZONF NUMBER >1 3 12 12 1 4 1 1 13 13 1 4 4 4 12 12 I 4 6 fa 12 14 1 4
ZONE WiMRFR -AT EACH MESH INTERVAL
S P E C IF IC A T IO N FOR l a y e r NUUBtR 1
i 2 ?- 4 ■» 6 7 8
1 » „ i 1 1 1 1 1 1 1i 1 1 1 1 I 1 1 .......... ' '
! a i ! 1 1 1 1 I 1
4 1 1 1 1 1 1 1 15 2 1 1 1 1 1 I 16 2 2 2 1 I i 1 17 ? ? 2 2 1 1 1 18 2 2 2 1 j 1 19 2 2 2 2 2 2 2 2
10 2 2 2 2 2 2 2 ?11 ? 2 2 2 ? 2 2 212 2 ? 2 2 3 3 2 213 2 3 3 3 3 2 2 214 ■x 3 3 3 3 2 2 2Id 3 3 3 3 3 3 2 2
SPECIFICATION FOR LAYER NUMBER 2
1 2 3 4 5 6 7 8
1 1 1 1 1 1 I 1 1? 1 1 1 1 1 1 1 13 1 1 1 1 1 1 1 14 1 1 1 1 1 1 I 15 2 1 1 1 2 1 1 1
2 i 2 1 1 1 1 " T " ''7 2 2 2 2 1 «ft I 18 2 2 2 2 I I I t9 2 ? 2 2 2 2 2 2
10 2 2 2 2 2 2 2 211 2 2 2 2 2 2 2 ?12 2 2 2 2 * 2 2 213 2 3 3 3 3 ? 2 214 3 3 -j 3 3 2 2 215 3 3 ■* 3 3 3 2 2
S P E C IF IC A T IO N FOR LAYER NUMBER 3
1 2 ? 4 5 6 7 8
1 1 1 1 1 1 1 12 1 1 i I 1 i 1 13 1 1 i 1 1 i 1 I4 1 ! i 1 I L 1 15 2 1 i 1 1 1 1 16 •» 2 2 I 1 1 1 I7 7 2 2 2 1 1 I 18 * £ 2 2 1 t 1 19 2 2 j 2 2 2 2 2
T o 2 2 2 2 2 2 2 2U . ? 2 2 2 2 2 2 212 2 2 2 2 3 2 2 213 2 3 3 3 3 2 2 ?14 3 i * 2 2 215 3 3 3 3 a«■ 3 2 2
S P E C IF IC A T IO N FOR LAYER NUMBER 4
1 2 3 4 5 0 7 8
1 ?. ? ? 2 2 ' 2 ?. 22 2 2 2 2 2 2 2 23 2 2 2 2 2 2 2 2
5u >
« 7 2 2 2 2 ? 2 ?5 2 2 ? 2 2 2 26 2 * 2 i * * ?7 2 2 ? 2 2 2 2 28 2 2 2 2 2 2 2 79 ? 2 2 2 2 2 2 7
16 i 2 * 4 2 i 2 "t l 2 2 2 2 2 2 2 2
“ 12 2 2 2 2 3 2 2 <;13 2 3 3 4 2 2 2
' U 3 3 1 i 3 2 ? 215 3 3 3 3 3 3 2 2
F I S S I O N SOURCE D I S T R I B U T I O N ANC SUM P . 7t»bCC 0 .2 3 * 0 0 C . 01000 0 . 0 ________ UUO________ _____________ I . 0000 J
c o r f s t q b a c e o i f f f b e n c e ( h q r q s i e q u a t i o n c c n s t a n t s i / o i n s t e a d o p s t q w e o 9 n z r _________________________
EQUATION CONSTANTS MILL BF STORED ON 1/0 LCG ICAL IS
NUMBFP OF-------COLUMNS, RO*S, PLANES. CROUPS. U P 5 C A T. OOWNSCAT, k E G IC N S , ANO ZONES U 15 * 6 U 2 ©V 3
MEMORY LOC ATIO N S RES**VEl> FOK OAT A STORAGE------- 40CCOMEMOBV LOC ATIONS IISSO FOR Ttil S PROBLEM----------------- I f 2**MEMORY LOC ATIO N S NOT USED--------------------------------------------------- 29>56
E— 1 ->3 ■P-
T H U T A -R -Z CASE TO CCMPARF TN I AGONAL, U K f - lW E L T H h IT H BLACK ABSORBER8X15X4X6 GROUP, 2880 P C IN TS STSEA* OF C I T A T I O N CASES
L I N E RELAXATION WILL ME DONE CN ROWS - 3 INNER I T E R A T I O N S )ORNL 72
I T E r A TIP N 1
FLUX CHANGE 2 .1 7 8 9 4 ? 00
HETA 1 .0 0 000
MU-14 .3 5 7 3 9
M U -2 -1 . 9 2 4 8 8
MU-30 . 0
It0 .4 2 3 4 5 0
z 3 .5 0 9 5 ‘JE 00 1.76171 5 .1 2 0 2 7 0 .0 3 8 9 5 0 .2 9 1 4 4 0 .5 5 3 5 5 6% 6 .6 " 1 3 7 e CO 1.61512 6.48232 0 .0 0 1 3 9 0 .9 0 1 5 4 0 . 6 3254o4 5 .9 5 0 6 1 F —01 1 .5 3 6 4 9 0 .6 8 5 2 3 0 .1 6 8 5 1 0 .5 5 1 JO 0 .6 8 3 9 9 95 - 4 . 0 1 7 2 8F-01 1.4973 7 - 1 . 0 7 6 8 3 -0 . 1 1 3 0 0 0 .4 1 4 6 2 0 .7 0 4 9 3 36 - ? . ? 2 l 6 6 t - 0 1 l .4 7 8 o 5 C . 34576 C . 41413 0.4 6 0 8 1 0 .7 1 3 8 2 87 - 1 . 1 1 632E-01 1 .4 6 9 8 5 0 .3 6 9 1 9 0 .5 0 5 3 3 0 .4 7 9 4 1 0 .7 1 8 1 2 /8 - 5 . 1 3 2 M F - 0 ? 1.4 6 5 7 6 0 .4 0 8 4 3 0 .4 9 3 2 5 0.4 5 9 3 Q 0 .7 2 0 1 1 89 - 2 . 3 7967 F -0 ? 1 .4 6 3 0 6 0 .4 3 4 8 7 C . 48734 0 .4 5 7 3 9 C » 721029
10 - 1 . 1 2 6 7 3 E - 0 2 1.4629B 0.46221 0 .4 8 6 2 3 0.4 5 8 8 1 0 .7 2 1 4 4 911 -5 . 4 2 7 9 6 F - 0 ? 1 .4 6 7 5 7 0 .47632 0 .4 8 B 5 7 0 .4 5 4 7 4
-5 .b 8 6 & V fc -6 * txTftAPuLAT ION WITH C.4321 0 . 72182817 l . 5 ' i f e a ! E - r 4 1.0 0 0 0 0 - 0 . 02761 - 0 . 1 2 4 1 7 0 .8 8 6 8 5 0 .7 2 1 3 2 0
— n -------- . 0 0 2 V 5 E-0 4 1 .4 6 7 3 0 - 0 . 6 6 5 4 5 - 0 . 6 3 4 8 8 - 0 .0 5 9 0 2 0 .7 2 1 8 2 014 - 6 . 5 9 8 2 3 E - 0 5 1 .4 b ? ? 6 0 .6 5 8 0 8 0 .3 3 3 3 6 0.9 4 3 9 1 0 .7 2 1 8 1 9
END OF EIGENVALUF CALCULATION - ITE R A T IO N T IK E 0 .1 7 6 MINUTES
CONVFRG'NCE 1N0ICAT KIM BY M IN IM IZ IN G THE SUM OF T)iE SOUAKES OF THE RESI& JES - R c L A T IV E ABSORPTION 0 .9 9 9 9 9 1 4 K 0 .7 2 1 8 1 1 5
LEAKAGE 4 .1 9 2 1 2 F 05 TOTAL LOSSES 1 .6 3 8 9 2 E 06 TOTAL PRODUCTIONS 1 .1 8 3 0 J 6 06 REACTOR POwERIWATTS) 1 .0 1 6 1 9 E 09
A D JO IN T PROBLFM FOLLOWSI T E ^ A f ION FLUX CHANCE ■ BTTX .....‘HTFT “ Mu-2” riu-5 K
1 1 . 14888E ?0 l.OOOOO********** ■- 0 .6 4 8 7 4 0 . 0 0 .7 2 1 8 1 92 1.85&86E *1 1.76171 18 .5 5 7 9 8 1 .6 8 5 5 3 c.c 0 .7 2 1 8 1 93 1 .7 5 9 1 4 F 01 1 .6 1 5 1 2 1 8 .5 3 9 2 6 0 .1 0 3 6 9 0 . 0 0 .7 2 1 8 1 94........ 5 . 4 9 2 * ^ - 0 1 1. £3 649 0* 58052 0 .1 7 9 2 4 0 . 0 0 .7 2 1 8 1 95 1 .1 9 8 8 4 F -0 1 1 .4 9 7 3 7 0 .3 * 8 1 3 0 .1 8 6 6 6 0 . 0 Q .7 2 l t f l 96 S.6&^6if-d? 1 ■ l .A r a t r 0. 3414^ 0.24252” u.o 6 .7 2 1 8 1 97 1 .2 1 6 3 2 F -0 2 1 .4 6 9 8 5 0 .3 4 4 5 2 0 . 2 V 968 0 . 0 0 .7 2 1 0 1 9ft - - 4 7 \ 8 5 W -< 5 T ~ 1.41*576 0 .3 6 4 9 8 0 .2 1 7 8 4 0 . 0 0 .7 2 1 8 1 99 1 .8 4 6 3 1 E -0 ? 1 .4 6 3 8 6 0 .4 2 2 8 1 0 .3 8 0 9 0 0 . 0 0 .7 2 1 8 1 9
Id 8 .3 5 4 1 9 F -0 4 1.4 6 2 9 8 0.45331 0 .4 6 4 8 6 0 . 0 0 . 7 2 U i y11 3 .8 6 2 3 8 F -0 4 1 .4 6 2 5 7 0.4 6 2 7 1 0 .6 8 4 4 0 0 . 0 0 .7 2 1 8 1 912— ....... U t t 3 ( J 3 6 - b 4 1 .4 6 2 3 8 ■ ' c ; ^ 5 W ... 0 .6 5 2 0 1 0 . 0 O . V i l 8 1 913 7 .7 2 4 7 6 E - 0 5 1 .4 6 2 3 0 0 .4 3 5 5 6 0 . 74586 0 . 0 0 .7 2 1 0 1 9
END OF A D JO IN T C A L C U IA TIO N - ITER At ION TIME 0 . 1 1 7 MINUTES
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES CF THc RESIOUbS - R E L A T IV E ABSORPTION 0 .9 9 9 9 8 0 3 K 0 .7 2 1 8 0 7 9
GROSS NEUTRON BALANCE
GPP L F T LEAKAGE TOP L FA KA tf K I I LEAKAGE BOT LEAKAGE FKT LEAKAGE 8AK LbAKAGE B**2 LOSSES 1/V LOSS XENON LOSSi 0. 0 0 . 0 6 . 6 ’ ' 1.64030E 6 J 1.23652E 05 0 .0 0 . 0 0 . 0 0 .02 o.e P.C r-.c 6 .5 8 1 6 6 E 03 1 .7 1 7 1 7 E 05 0 .0 O .C 0 . 0 0 . 0I 0*0 0 . 6 0 . 6 4.44S83E til ' 8 .6 S 6 4 5 S 04 0 . 0 0 . 0 0 . 0 0 . 04 0 . 0 0 . 0 0 . 0 1 .2 5 5 6 5 E 03 2 .1 2 3 3 7 E 04 0 . 0 0 . 0 0 . 0 0 . 0S f l .9 0.* r . c 3 . 79576E 02 i . r m x a s - 0 . 0 o .x 0 . 0 0 . 06 0 . 0 0 . 0 0 . 0 5 .5 3 6 6 9 E 01 5 .6 8 0 0 2 E 02 0 .0 0 . 0 0 . 0 0 . 0
(SUM 0 .0 0 . 0 0 . 0 1.43&64E 04 4,04d55e C5 0 .0 0 . 0 0 . 0 0 . 0
GRP ABSORPTIONS I 2 .107& 4E 05
1 — J . f W l W f i* 4.020396 05
O U T-S C A TTE R 9 .0 2 9 78C 65y . ? ? o r « o r3 .0 3 * 5 2 6 05 i.oidCaf 05
y i u H U i.23Va?E 06
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S P E C IF IC A T IO N FOB LAVER NUN*ER ? ------------ - - —
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S P E C IF IC A T IO N FOR LAYbR NUNREK 3
1 2 3 4 5 6 7 8 9
1 2 2 2 2 2 2 2 2 22 2 2 2 2 2 2 2 2 Z3 2 2 2 2 2 2 2 2 ?4 1 2 2 2 2 2 2 2 2 .........5 2 2 2 2 2 2 2 2 26 2 2 2 2 2 2 2 2 27 2 2 2 2 2 ? 2 2 2t 2 2 2 2 i 2 2 2 ?9 2 2 2 2 2 2 2 2 2
s p e c i f i c a t i o n f o r LAYER NUNHER 4
1 2 3 4 5 6 7 8 9
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S P E C IF IC A T IO N FDR LAVER NUMBER S
1 2 3 4 5 6 7 8 9
1 2 2 2 2 2 2 2 2 22 2 2 2 2 2 2 2 2 23 2 2 2 2 2 2 2 2 24 2 2 2 2 2 2 2 2 25 2 2 2 2 2 2 2 2 26 2 2 2 2 2 2 2 2 27 2 2 2 2 2 2 2 2 2fl 2 2 2 2 2 2 2 2 29 2 2 2 2 > 2 2 2 2
s p e c i f i c a t i o n f o r LAVER n u m b e r 6
I 2 3 4 5 6 7 8 9
1 2 2 2 2 2 2 2 2 22 2 2 2 2 2 2 2 2 23 2 2 2 2 2 2 2 2 24 2 2 2 2 2 2 2 2 25 2 2 2 2 2 2 2 2 26 2 2 2 2 2 2 2 2 27 2 2 2 2 2 2 2 2 28 2 2 2 2 2 2 2 2 29 2 2 2 2 2 2 2 z 2
s p e c i f i c a t i o n f o r LAVER NUMBER 7
1 2 3 4 5 6 7 8 9
1 2 2 2 2 2 2 2 2 'i2 2 2 2 2 2 2 2 2 23 2 2 2 2 2 2 2 2 24 2 2 2 2 2 2 2 2 25 2 2 2 ? 2 2 2 2 36 2 2 2 2 2 2 2 2 27 2 2 2 2 2 2 2 2 2fi 2 2 2 2 2 2 2 2 29 2 2 2 2 2 2 2 2 2
S P E C I F I C A T I O N FOR LAVER NUMBER 8
1 2 3 4 5 6 7 8 9
1 .7 2 2 2 2 2 2 2 ?
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• S P E C I F I C A T I O N 5GK LAYfcR NUHPT. 9
1 ? 3 4 * 6 7 8 9 10
1 3 3 3 1 * 3 3 3 3 32 * 3 3 3 3 3 37 r *3 * 3 3 3 3 3 3 3 3 34 3 3 1 3 3 3 3 3 '3 "T "5 3 3 3 3 3 3 3 3 3 36 3 3 3 3 4 3 3 3TT7 3 3 3 3 3 3 3 3 4 *8 * ‘1 3 3 3 3 3 3 3 T T9 3 3 3 3 3 3 3 j 3 «
0 0V O
S p e c i f i c a t i o n f o it l a v c « numsck 10
t 2 J 4 “5 0 T ~3' * t *
1 3 3 3 3 3 3 3 3 3 32 3 3 3 3 3 3 3 3 3 3•» 3 3 3 3 3 3 * 3 3 34 3 3 3 3 3 3 3 3 3 35 % i - y — j — 3 * * T6 j 3 3 3 3 3 3 3 3 37 3 3 3 ? 3 a 3 3 3 38 3 3 3 3 3 3 3 3 3 39 3 3 3 3 3 3 3 3 3 3
10 a 3 3 3 3 3 3 3 3 3
F IS S IO N SHURCF U 1S T R IB U H O N AND 'SUM r ,V 3 ^ 2 C Q.0t»5i>0 C .G t O s C C .O l.OUUOO
CORF STORAGF DIFFERENCE tWORQSI EQ UATION CCNSTANTS I/O INSTEAD OP STORED 1 2 TBS
EOtfAT lf)N CONSTANTS H i t t OE STOKED 1 « CORE
NUHUFft OF -COLUMNS» PQWSt f t ^ N E S t GftOUFS. U P S C A T, QUWNSCAT, frEGICNS, ANO ZUN6> 10 10 10 * 0 0 2*3 7
HEM9RY LOCATIONS RESEKVEO FOR OAT A StOP A Gt-------M E M O R Y LOCATIONS USfO FO^ T H I S PROBLEM---------------------- 2u*ie?MEMORY LOCATIONS NOT USED----------------- --------------------------------- 11013 ____________ ____________________________________________________________________
***********ARNING i n p u t s p e c i f i e d o ow m scattep * c h a s been ch angeo t o a c t u a l o o ^ n s c a t t e r > 2
3 -0 WARD FFTF PROBLEM IN RgQUCEO HESH. FEWER GRCLPS10X10X10X4 GROUP, 4000 P O IN TS STHtftt* OF C 11 AT ION CASES OIWL 72
L I N E RELAXATION WILL PF DONE OH ROWS - 3 INNER I T E R A T I O N S !I T E r STTTWk T l d i T T H T N T j r bET A MU-1 K U -2 MU-3 K
1 1 .8 6 5 5 7 E 00 l.ocooo 3 .7 3 1 2 3 - 1 . 9 9 3 5 1 0 «C 0 .6 3 9 2 4 72 3 .0 1 2 9 5 E 00 1 .7 8 5 1 5 4 . 62798 0 .0 0 3 2 4 0 .5 3 9 4 3 0 .9 3 8 0 6 93 2 .5 0 7 9 5 E 01 1 .6 4 6 3 0 3 3 .4 0 3 4 1 0 .0 0 4 9 4 0 .0 9 1 4 4 0 .9 6 2 3 2 64 1.35279E 01 1 .5 6 7 5 0 1 4 . Co731 0 .0 1 7 2 4 0 .1 8 7 9 2 0 .9 7 2 0 4 15 7 .0 8 7 8 7 E -0 1 1.52605. 0 .7 6 1 1 8 0 . 1 1 2 5 0 0 .8 4 4 8 8 0 .9 8 1 3 7 76 - T . I W 7 E - 0 T 1.5 0 5 1 1 - 6 . 28*11 5 - 0 . 3 2 0 7 6 0 .3 3 9 1 5 0 .9 8 6 2 6 47 - 5 .5 0 3 8 6 E -0 2 1 .4 9 4 7 5 U . 40386 0 .5 6 0 2 9 0 .4 8 0 9 6 0 .9 8 9 4 0 88 1803I E —02 1 .4 8 9 6 8 - 0 . 5 4 6 0 3 - 0 . 6 2 0 1 7 0 .4 7 1 2 7 0 .9 9 1 5 3 39 2 .0 4 1 3 4 E -0 2 1 .4 8 7 2 0 0.6t>22B 0 .5 8 6 3 5 0.4547<i 0 .9 * 2 0 7 5
10 1 .3 2 1 4 1 E -0 2 1 .4 8 6 0 0 0 .6 6 0 6 4 0 .6 2 4 6 4 0 .4 1 9 5 1 0 .9 9 3 7 5 411 8 . 6 3 2 6 6 E - " 3 1 .4 8 5 4 2 C . 66192 0 .6 4 5 7 8 0 .3 0 6 3 0 0 .9 9 4 3 3 112 5 . 6 6 7 6 9 E -0 3 1.4 A 5 1 4 A . 66221 0 .6 5 6 C 4 -0 . 1 2 3 2 0 0 .9 9 4 7 1 0
. 13 3 . 7 2 9 8 2 E -0 3 1 .4 8 5 0 0 0 . 6 u l 81 0 .6 6 2 5 9 5 .3 9 4 5 b7 .2 8 4 6 3 6 -0 ? EXTRAPOLATION WITH 1 .9 6 0 3 0 .9 9 3 4 5 0
14 2 .0 0 2 7 2 P -0 4 1 .0 0 0 0 0 0 .0 5 3 8 9 0 .0 2 9 5 6 3 .0 8 4 9 6 0 .9 9 5 4 4 715 i . t e l f t t - o 4 1 .4 8 4 9 0 1.0 0 9 7 2 1 .6 0 3 5 / 0 .5 9 9 6 7 0 .9 9 5 4 4 816 1 .5 0 6 8 1 E - 0 4 1 .4 8 4 8 9 P . 74543 0 .4 C 1 8 2 0 .9 7 1 5 7 0 .9 9 3 4 4 717 '9.1552'fP-OT U 4 d 4 B 8 0 .6 U ? 6 9 0 .6 9 3 2 $ 0 .9 2 1 3 0 0 . 9 9 5 S4f
END OF (EIGENVALUE CALCULATION - I T E R A T IO N T IHfc 0 .< O d MINUtES
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF T h t SUUAfeES GF I h E f t tS l tU E S - R E L A T IV E ABSORPTION G.99999t>3 K 0 .9 9 3 4 3 3 *
LtaKAGC 5.R210IT 17 IOTAL l OSSES S7F^Tc7 T T 3 V u t a l HOOuClf nJnS 5751u99fc~T5 r e a c t o r p o w E r i n a i t s i 4 .12371E 08
5B0 S S'H g tiTTON S'g fT O fc -------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------
7TRP CTT LEAKAGE TOP LFAlsAGE R I T LEAKAGE BOT LFAKAGfc F nT T E S R a BE BAK LEAKAGE 8**2 LOSSES l / V LOSS* XENON LOSS1 0 .0 ______________ 0 .0 _______________________________________ 1 .0 1 2 7 3 E 17 3 .8 0 0 5 5 E 16 C .C _3 .3 0 0 a 0 E l o 0 » 0 _____ 0 . 0 ___________ 0 . 0
~2 0715 b.o 1 .8 7 9 $ 6 f 17 6775521c“ 16 37o 6 .7 B 9 7 4 E l b oTE : oTo 0 . 03 0 . 0 0 . 0 1 .3 4 5 2 3 E 16 5 .9 9 4 9 6 E I S 0 . 0 5 .9 9 S 8 1 E 15 0 . 0 0 . 0 0 . 0
------ 070--------------------- 070--------------------- 2 .g T W BEH> I."<g7W l~n J TC----------------------lb '6 .(5 ---------------------------------------- O --------------------- C.~0
SUM 0.0--------------------0r 5--------------------3 .? W i r T 7 — 1.26552FT7— i5TT3-------------------1.^6CU6¥ T 7 " o.u--------------------u.'o------------------o^T
GRP ABSORPTIONS O U T -S C A TTER SOURCE IN -S C A T T E R TO TAL LCSSES TOTAL G AlH S FKCD/AtsSCRP“ I--------q.2<.21<»E IT 3.15T K E 10 4.24ZaZt ~lti 0.0------------------------4.2i2ibG U 4.242S7T R>-------------------------------------------------------------- ^ l i a03E~ UU—
2 1 .9 1 9 4 1 E 18 1 .1 9 3 6 7 E 18 2 .9 7 4 7 9 C 17 3 .1 3 9 3 3 E 18 3 .4367BE 18 3 .4 3 6 8 1 E I d 1 . 0 4 7 6 U 00“ 3-------47777Z3TT7 S77TH75n7 lT35?50rT5 T7T9J6?FTS TTTJFoSFTB rTRSoSFTw------------------------------------------------------7wfc396E~oT
4 6 . 1 6 U 0 E 17 C .O ______________0^_2_____________ 6 .7 1 6 6 2 6 17 6 .7 1 8 8 C E 17 6 .7 1 » d 2 E 17______________________________________4 .2 9 3 6 0 6 - 0 1
SUM 3 .9 5 9 4 5 E 18 5 .0 0 4 8 9 F 18 4 . 54166E 18 5 .0 0 4 8 9 E 18 9 .5 4 6 5 0 E 18 9 .5 4 6 3 6 E 18
END OF CASE - TOTAL CPU TIME WAS 0 .2 5 MINUTES TCTAL CLUCK T IM E WAS 0 . 5 7 MINUTES *******************?«**
* * * «* * * «* TH IS JOB MAS RUN ON 0 3 -1 1 -7 2 CN THE IBM 360/91
3 -0 CASF C A U E O CL 46 ( K i i P L I , DATA IN PUT FROM D IS K FORCEU.__________________13X13X18X1 CROUP, 9126 P O IN TS STREAM OF C I T A T I O N CASE.; ORNL 72
GENERAL CONTROL INPUT - SEC TIO N 001
ft 0 * P D 0 0 0 0 t ~f> 6 “ 7. 0 0 0 0 0 1 u 0 0 I 01 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 Q u 0 0 0 0
200 lOO *15 t $ t 0 1 .5 0 0 0 C 0 E OP 5 .0 0 0 0 0 0 6 -0 1
0 0 9 .9 9 9 9 9 9£
609
0 0 0 9 .9 9 9 S 9 9 E
023
U0 . 0
0 0 0 20 6 I .OUOOOOE
12uo
6 12 24
NEUTRON FLUX PROBLEM OESdJl-PT ION - SECTJON 003
P 0 0 C 11 P 0 0 0 0 0 0 1 1 O O O O O O O U O O9 . 9 9 9 9 $ 9 f : - ' 0 r i . i )0 ( j0 0 < iE -0 50 . 0 a. o
9 .9 99999E- 0 5 9 . 99999VE-O'V
9 .9 9 9 S S 9 E -0 5 I . 0000 COE. 00
9 .9 V V V V 9 E -0 5 0 . 0 1 .2 5 0 0 0 0 6 -0 1 0 . 0
L E F T ,T O P ,R IG H T ,B O T T O M ,F R O N T ,BACK BOUNDARY C O N D ITIO N S ARE4 , 6 9 2 0 0 0 E -0 1 4 .6 9 2 0 0 0 E - 0 1 0 . 0 0 . 0 4 . 6 9 2 0 0 0 E -0 1 4 .6 9 2 0 0 0 E - 0 1
THREE DIMENSIONAL SLAB GEOMETRY ( X , Y « Z ) WIDfH 7 .5 3 2 5 0 U E 01 HEIGHT 7 . 532500E 01 DEPTH 1 .2 4 b S 0 0 E C2
REGIONPTS
S P E C IF IC A T IO N S REGION WIDTH
3 9 . 000(It)05 00 4 2.65300& E O l 4 - r."t536SDF"ffT— ' 2 I . 326500* 01
p t S3
■RECTOR HElGttt 9 . OOOOOOE 00 4 2 .6 5 3 0 0 0 E 01 4 2.653O0OE 01 2 1 .3 2 6 5 0 0 E 01
PTS REGION DEPTH3 9 . OOOOOOE 00 6 5 .8 4 2 0 0 0 E 01 6 4.e25999f= 01 3 9.COOOOCE 00
r a n TT. t o f t t n ---------------------v- q i h . p m m s " 1 3 ---------- -------------R n r r w i m r ' i i
1>r5T«CC5 TQ TfFSH INTERVAL IWrt'ftFACET
— j - 2
B I S T .? .0 0 0 3 f>. 000 4 9 ,0 0 0 5 1 5 .6 3 2 6 2 2 .2 6 5 7 2 d .8 9 7 e 3 5 .5 3 0 9 4. ' . 162 10 4 ' , . 7 «
T I ‘ 5 ^ .4 'T T " 12 6 2 .0 6 0 13 1% f & . 3 iS
I f i s t ;2 3 .0 C 0 3 6 .0 0 0 4 9 .0 0 0 5 1 5 .6 3 2 6 2 2 .2 6 5 7 2 4 . <19/ d 3 5 .5 3 0 V 4 2 .1 6 2 10 4 8 .7 9 5
11 5 i . 4 » f 12 6 * .0 6 0 13 6 8 .6 9 2 14 7 5 .^ 2 5
KB "515Y "2 3 .0 0 0 3 O .P0P 4 9 .0 0 0 5 1 8 .7 3 7 6 2 o .4 / 3 7 3 0 .2 1 0 « < 7 .9 * 7 9 5 7. 603 10 6 7 .4 2 0
11 7 S .4 6 3 l k 8 3 . 50 7 l i 9 1 .5 5 0 14 99.i>93 IS 1 3 7 . 6 3 ? " 16 t l 5 . 6 o O 11 i l b . 6 6 0 l a 1 2 1 . 6 0 0 1* 124.61)0
D ISTAN CES TO T LUX PO IN TS
' J " 1
t n s r .1 .5 0 0 2 4 .5 0 0 3 7 .5 0 0 1 2 . a 16 5 1 8 .9 4 9 6 2 5 .5 8 1 1 3 2 .2 1 4 8 3 8 . o46 9 4 5 .4 7 9
to ~ 5 ? : t r r ' 11 5 6. 744 12 6 5 .3 7 6 " i s ... i r . T w —
t — f n m ------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------ --------------------------- ----------------------------------------------- —1 1 .5 0 0 2 4 .5 0 0 3 7 .5 0 0 4 1 2 . 31b 5 1 8 .9 4 9 i 2 5 .5 6 1 7 3 2 .2 1 4 ti 3 8 .8 4 6 9 4 5 .4 7 9
10 T ? . n l ' Y? 6 ',.T 76 l T - rzT v e s ~
Kfi PIST 1 1 .500 2 4 .500 3 7.500 4 1 3 .8 6 b V 23.&U5 6 3 3 .3 4 2 i 4 5 .0 7 # tt 52.M 15 9 * 2 .5 * 2
10 71.442 11 7V.AB5 I? 87.52c 13 95.512 K 1 0 2 .6 1 5 15 U l . o S b l o 1 1 7 .1 8 0 I t 12C . U O 1* 123*196
ZONE INPUT BY EC ION
PLANE MUMPER 1 I 1
11
1 1 1 1 1 I
11
1 1 1' 1
PL«n|F 1 I 1
y '1
i i i 1 3 2
r " ...........2
1 2 ? 4
PLANF NlHBEft 5 5 5 55 5 f 5 7 6
&6
— 5 6 " 6 "~8~~
P U N E NUFBFJT 5 5 5
4 '5
5 5 b 5 5 5
S ..................... ...........5
V Ou >
Z'ON? «5JMfiET"Sr M C H "R ,E T R " I R T ? ’*CVJtr‘
T w r r n r m d r T T j i r - L A V E R 'w a s t s — i—
SPPCI FirATrn*g M R LAVER MUMitcK 2-------------------------
-----1 ?.3 i, r ~ T.T 'l.¥ 10 ITT? 11_j----- f -J j — r - r— j-'-y - r j - -r ~ y r
2 1 1 1 1 1 1 1 1 1 1 7 . 1 11--- 1— K— — l— I— r"i— i— £--r -T -T -4 1 1 1 1 I I 1 1 1 1 I 1 1
5p'en?Tr Atl(JN SD«“
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_ _ _T — ~ r ~ r r i _ T
2 j 1 1 i 1 i i i i i i 1i I i t i i I Y T T i
4 l 1 1 1 1 ! 1 1 i 1 1 l5 r 1 1 l i 1 ~ I ' "1 l T ~ T T6 i 1 t 1 1 1 1 1 * 1 1 l7 i t l i l " T 1 ! t i r I8 i 1 1 1 1 1 1 I I i i l9 r i 1 1 1 "“I T~ 1 I i I 1
10 i I 1 I J 1 1 t ! l i lu r 1 I l l ~ i r~ T ~ T n T1? «* 1 1 I l 1 1 1 I i t lra ■ t 1 I 1 i t i r i i t
sFfciTicTrTrrir- TT vT w' NOiJRpr *
1 2 1 4 3 6 7 8 10 11 12 IS
i i t I I 1 I I 1 t I 1 I 1? l a 1 1 1 1 I 1 1 1 1 1 13 l 1 I 1 1 1 i 1 1 1 1 I I4 i ! ! 1 J ! i 3 3 3 3 2 25 l 1 1 i 1 1 i } ■» 3 3 2 2A l 1 1 I 1 > 1 ? 3 ■» 3 2 27 l 1 \ 1 1 t I 3 ~r~ \ i 2 28 l 1 1 3 ? •» 3 2 2 > 2 2 29 i 1 I 3 3 3 3 *>c 2 ) 2 2 2
10 l 1 1 3 3 3 j z 2 2 2 2 2u 1 1 I 5 3 1 J •> ? 2 2 2 i12 i I ! 2 2 2 2 2 2 2 2 4 •tT5 ----------- 1— I— I— 2— 2— 2— 2— ?— Z— ?— 2— SS— 4
bPEnTTCTT ■ftM P7Tft "RTfssrir 4
1 i 4 *> 6 / a *r M 11 12 13
I I l l i t i * 1 I i 1 12 1 I I i 1 i l 1 1 l 1 13 I t 1 » 1 i ■» I 1 1 14 1 1 1 i 1 i 3 3 3 3 2 2
i " 1 r “ i l 1 l i T " TT ? 2 I6 I 1 1 i l i 3 3 3 3 2 27 I I 1 i I t J J 3 J 2 2a 1 I 3 3 3 i 2 2 2 2 2 29 i I 3 3 3 3 2 ?. 2 i 2
10 I t 3 ■> * ■* ? 2 ? 2 2
H
1! 1 1 1 3 3 3 3 2 2 2 2 2 212 1 1 1 2 2 2 2 2 2 2 2 4 413 1 1 1 2 2 2 2 2 2 2 2 4 4
“S P f t l f lCAT ION FOR LAYER NUMftER 6
1 2 3 4 5 6 7 8 9 10 11 12 13
1 1 1 1 1 1 1 1 1 1 1 1 I 12 1 I 1 *A 1 1 1 1 1 1 1 1 13 1 1 1 1 1 1 1 1 1 I 1 1 14 1 1 1 1 1 1 1 3 3 3 3 2 25 1 1 1 1 1 1 1 3 3 3 2 26 1 1 I 1 1 1 1 3 3 3 3 2 27 1 1 1 1 1 1 1 a 3 3 3 2 28 I 1 1 3 3 3 3 2 2 2 2 2 29 1 1 1 3 3 3 3 2 2 2 2 2 2
10 1 1 1 3 3 3 3 2 2 2 2 2 211 1 1 I 3 3 3 3 2 ?. 2 2 2 212 1 1 1 2 1 2 2 2 2 2 2 4 413 1 1 1 2 2 2 2 ? 2 2 2 4 4
~5 f e t t F r o m ON FOP LAYeR NUMBFir 7
1 3 4 0 6 1 H 9 lo 11 12 13
1 1" 1 ' I 1 I 1 1 1 1 1 1 12 1 1 1 1 1 1 1 1 1 1 1 13 1 1 1 1 I 1 1 1 1 1 1 14 1 1 1 1 I 1 3 3 3 3 2 25 1 1 1 1 1 I 3 3 a 3 2 26 1 1 1 1 1 1 3 3 3 3 2 21 1 1 1 t I L * * * 4 2 28 1 1 3 3 1 3 2 2 2 2 2 29 1 1 3 3 3 3 2 n ? 2 2 2
10 1 1 3 3 3 2 2 2 2 2 211 i 1 3 3 3 3 2 2 2 2 2 212 1 1 2 2 2 2 2 2 2 2 4 413”
. . . . 11 2 2 2 2 2 c 2 2 4 4
■ S p e c i f ic a t io n f o r l a y f r .^umsfk 8
i — 2— t ' - 4— -y "5— t s n r m n r
1 1 1 I 1 1 I 1 1 1 1 1 1 i2 1 1 1 1 1 I 1 1 1 1 1 13 1 1 1 "1 1 1 1 1 1 1 1 1 14 1 1 1 1 1 1 1 3 3 3 3 2 25 1 r y r 1 1 1 4 3 3 2 26 1 i i i 1 1 1 3 3 3 3 2 27 1 i i i 1 1 1 3 3 3 2 t8 1 1 l 3 3 3 3 2 ? 2 2 2 29 1 1 1 3 3 3 3 2 2 2 2 2 2
10 1 1 1 3 3 3 3 2 2 2 2 2 211 1 1 1 3 i 3 3 2 2 2 2 2 212 1 1 1 2 2 2 2 2 2 2 2 4 4I? 1 1 1 2 2 -2 2 2 2 2 4 4
MVOv n
SPECIFICATION FOR LAYER NUMiJtR 9
1 2 3 4 5 6 7 8 9 10 11 12 13
1 1 1 I 1 1 1 1 I 1 I 1 1 I2 1 1 1 1 1 1 1 1 1 1 1 i 13 1 1 1 1 1 1 1 I 1 1 1 1 14 1 1 I 1 1 1 1 3 3 3 3 2 25 1 1 I 1 1 1 1 3 3 3 3 2 26 1 1 I 1 1 1 1 3 3 3 3 2 27 1 1 1 I I 1 1 3 3 3 3 2 28 I t I 3 3 3 3 2 2 7 2 2 29 1 1 1 3 ^ 3 3 2 2 2 2 2
10 1 ! 1 3 3 3 3 2 2 2 2 2 211 1 1 1 3 3 3 3 ? 2 2 2 212 1 1 1 2 2 2 2 2 2 2 2 4 413 1 1 1 2 7 e. 2 2 2 2 2 4 4
SpEcTFTcaTIqn T o r la y e r 'n u m re r 10
1 ? j 4 5 6 7 a 9 1° 11 12 13
1 5 5 5 5 5 5 5 5 5 5 5 5 52 5 5 5 5 5 5 5 5 5 5 5 5 53 5 5 5 5 5 5 5 5 5 5 5 ;> 54 5 5 5 5 5 5 5 7 7 7 7 6 65 5 5 5 5 5 5 5 7 7 7 7 6 6u 5 5 5 5 5 5 5 7 7 7 7 6 6T 5 5 5 5 5 5 5 7 t 1 7 6 68 5 5 5 7 7 7 7 6 6 6 6 6 69 5 5 5 7 7 7 7 6 6 6 6 6 6
10 5 5 5 7 7 7 7 6 6 6 6 6 611 5 5 5 7 7 7 7 6 6 6 6 6 612 5 5 5 6 6 6 6 6 6 6 6 8 8
T ? " 5 5 5 6 6 6 6 6 6 0 6 d ii
Sp e c if ic a t io n 1 FOR LAYER NUMBER i i
1 7. 3 4 5 6 8 10 11 W a
i 5 5 5 5 5 !> 5 5 5 5 t> 5 !>2 5 5 5 5 5 5 & 5 5 5 5 5 53 5 5 5 5 5 S 5 5 5 !> t> !>4 5 5 5 5 5 5 5 7 7 ? 7 6 6
- 5 "" B b y 5 5 !> S f 7 / / 6 66 5 5 5 5 5 5 7 7 7 7 b 67 5 5 5 5 5 5 5 ? 7 7 t 6 68 5 5 r 7 7 7 7 6 6 b 6 6 b9 5 5 5 7 7 7 T 6 6 6 6 6 6
10 5 5 5 7 7 7 7 6 6 6 6 6 bi l 5 5 i 7 7 ? 7 b 6 6 6 6 b12 5 5 b 6 6 6 6 6 6 6 6 8 813 5 ‘j 5 6 6 6 o 6 6 6 6 B 8
SPFCI FT CAT [TT^TTmrT^YFR" ,F'JUHf5TTR'12
-----1 ~ Y ~ \ -7J-—5- 6 7 8 -9 10 T l v T F 13
1 5 5 5 5 5 5 5 5 5 5 5. 5 52 5 5 5 5 5 5 5 5 5 b 5 5 5
Hvocr\
4 5 5 5 5 5 !> 5 7 7 7 7 b 65 5 5 5 5 5 5 5 7 7 7 7 b b6 5 5 5 5 5 5 5 7 7 7 7 6 67 b 5 5 5 5 b 5 7 7 7 7 b 68 5 5 5 7 7 7 7 6 6 6 6 b b9 5 5 5 7 * 7 7 b b b b b b
10 5 5 5 7 7 7 7 6 6 6 b b b11 5 b 5 7 7 7 / 6 b 6 b b b12 5 5 5 6 6 6 6 b b 6 b 8 813 5 b 5 6 6 6 b b b b b 6 8
s p e t i r n r r n o N ’ T n i r LftYgR NUMBER 13
i 3 4 b b 7 8 9 10 11 12 I S
i 5 5 S 5 5 5 5 !> b 5 5 3 b2 i 5 5 5 5 5 5 5 5 5 5 5 53 5 5 & 5 5 5 5 5 5 5 5 5 54 5 s 5 5 5 5 5 7 7 7 7 b b5 b § 5 5 5 s b 7 7 7 7 b bb 5 s> 5 5 5 5 5 7 7 7 7 b 6
"~7 5 b b 5 S 5 / / / / 6 b8 5 5 5 7 7 7 7 6 b b 6 b b
5 5 5 7 / 7 7 b 6 6 6 6 610 5 5 5 7 7 7 7 6 b 6 6 6 6r r 5 b S / f I 7 6 b 6 b b 612 5 5 5 b b 6 6 6 b 6 b B 813 5 b b 6 6 6 b 6 6 6 U “ 8
S P F c m C T T i r w T F m r U V E « 2 C J rr * 14
L 2 3 4 3 6 7 U *} 10 11 1<> T 3
' f “ b 5 5 5 6 5 5 5 b 5 a t> b2 5 b 5 5 5 5 5 5 b 5 5 5 5■4 5 5 5 5 5 5 5 b b 5 5 b 54 5 5 5 5 5 5 5 7 7 7 7 6 65 5 b b b b a b f I / 7 6 b6 5 5 5 5 5 5 5 7 7 7 7 6 6T -
5 5 b 6 b b S» 7 i 7 7 6 68 5 5 5 7 7 7 7 b b 6 6 b 69 5 ■J b 7 7 7 r b 6 6 b 6
10 5 5 5 7 7 7 F 6 L 6 6 6 b" T r _ b b b ; / f f b 6 b b 6
12 5 5 5 b 6 b 6 b b b b b 8..n ~ 5 5 5 4 6 6 6 6 b & 6 9 B
~T~T" ~ r * r 6 7 a"mri n n r
1 5" 5 5 5 5 5 5 b b b b "S'"1 T ~2 5 5 5 5 5 5 5 5 5 5 5 5 5
" 5 " T bib *> b !* b 5 b'TV5 5 5 5 5 5 5 7 7 7 7 6 6
5""' 5 5 5 5 ij & 5 7 / 7 ' 7 T “ o “6 9 5 5 5 5 5 5 r 7 7 7 6 6
' "7 * S " T " 5 5 y !> b J 7 7 1 6 68 5 5 5 7 7 7 7 6 0 6 6 6 6
9 5 5 5 7 7 7 7 6 6 6 6 6 610 5 5 5 7 7 7 7 8 6 6 6 b bu 5 5 5 7 7 r 7 6 6 6 6 6 612 5 5 5 6 6 6 6 6 6 6 b 8 813 5 5 5 6 6 6 6 6 6 6 6 8 8
Sp e c if ic a t io n for LAYER NUMRFR lb
1 2 3 * 5 b 7 8 9 10 XI 12 13
“ 1 5 5 & 5 5 5 5 5 5 5 5 5 52 5 5 5 5 5 5 5 5 5 5 5 5 53 5 5 5 5 5 5 5 5 5 5 5 5 54 5 5 5 5 5 5 5 5 5 5 5 5 55 5 5 5 5 5 5 5 5 5 5 5 5 5b 5 5 5 5 5 5 5 5 5 5 5 5 57 5 5 5 5 5 ii 5 4 5 5 5 5 58 5 5 5 5 5 5 5 5 5 5 5 5 59 5 5 S 5 b 5 5 5 5 5 5 b 1)
10 5 5 5 5 5 5 5 5 5 5 5 5 5l l S 5 5 5 5 5 5 5 5 5 i> 5 512 5 5 5 5 5 5 5 5 5 5 5 5 5
T T “ 5 5 5 5 5 5 !> 5 ii b b b i
SPECIFICATION FOR LAYER NUMBER 17
1 2 4 5 6 7 3 9 16 11 12 13
1 5 5 5 5 5 5 5 5 5 5 5 5 52 5 5 5 5 5 5 5 5 5 5 5 5 53 5 5 5 5 5 5 5 5 s 5 5 b 54 5 5 5 0 5 5 5 5 5 5 5 5 5S 5 $ b 5 5 5 5 b & 5 b 5 56 5 5 5 5 5 5 5 5 5 5 5 5 57 5 5 5 5 5 5 5 5 5 5 5 5 58 5 5 5 5 5 5 5 5 5 5 5 5 59 5 5 5 5 5 5 5 5 5 5 5 5 5
10 5 5 5 5 5 5 5 5 5 5 5 5 5T T “ 5 5 5 S s $ 5 5 i> i> b b S12 5 5 5 5 5 5 5 5 5 5 5 5 513 5 5 5 5 5 5 5 5 5 5 5 5 5
SPECIFICATION FOR LAYFR'UUMBERTIB------------------
I I 3 4 5 6 7 B 9 in U 12 13
1 5 5 5 5 5 5 5 5 5 5 5 5 52 5 5 5 5 5 5 5 5 5 5 5 5 5
~3------5- 5 - 5 ' 5—"5 5 5 5 " ’5 "5 V ” 5 5* 5 5 5 5 5 5 5 5 5 5 5 5 55 5 5 5 5 5 5 5 5 5 5 5 5 56 5 5 5 5 5 5 5 5 5 5 5 5 5
" T 1 5 5— 5 5— 5— 5— 5— 5— 5— 5— 5— 5— 58 5 5 5 5 5 5 5 5 5 5 5 5 5
“ 5---------5— 5— 5 5— 5— 5— 5— 5— 5— 5— 5 5— S'10 5 5 5 5 5 5 5 5 5 5 5 5 511 5 5 5 5 5 5 5 5 5 5 5 5 512 5 5 5 5 5 5 5 5 5 5 5 5 513 5 5 5 5 5 5 5 5 5 5 5 5 5
HVOCP
FISSION SOURCF DISTRIBUTION AND SUM 1.00000 0 .0 0 .0 1.00000
CORE STORAGE DIFFERENCE (WORDS! EQUATION CONSTANTS I/O INSTEAD OF STORED 25610
EQUATION CONSTANTS HILL BE STORED ON I/O LOGICAL 15
NUMBER OF-----COLUMNS, ROWS, PLANES, GROUPS, UPSCAT, OOWNSCAT, REGIONS, AND ZONES 13 13 la 3 0 1 64 a
HEHORV LO C ST Iflk S RESEAVEb FOR DATA SftifcA&e------ 46000-----------------------------------------------------------------------------------------------------------------------------MEMORY LOCATIONS USFD FOR T H IS PROBLEM------------------ 38460MEMORY LOCATIONS NOT USEO--------------------- ------------ T540
3-D CASE CALLED CLAG (K A P L). DATA INPUT FRUH DISK FORCED.13X13X18X3 GROUP* 9126
LINE RELAXATION WILL PEPOINTS DONE CN 1
STREAM OF CITATION CASES ROWS - 3 INNER ITERATION!S)
ORNL 72
ITERATION1
FLI/X CHANGE I . 7672IE 00
BETA1.00000
MU-13.53443
MU-2 -1 .87315
MU-30 .0
K0.718587
2 1.72618E 00 1.86575 2.70296 0.06761 0.23784 0.8727793 1.25282E 01 1.76328 19.78595 0 .CO164 0.25911 0.9295634 4* 97034F 01 1.69234 53.67061 0.00730 0.75968 0.9658495 6.23497E 00 1.64 647 6.36041 0.03574 0.62291 0.9886886 8.19992E 00 1.61813 9.51507 0.01920 0.63505 1.0028967 3.21992E 00 1.60109 3.61260 0.13698 0.64676 1.0118266 4.20973E 00 1.59101 5.51712 0.04741 0.65164 1.0174679 -5.21077E-01 1.58512 -0 .64486 -0 .15480 0.64611 1.021100
10 — 5 .37393E—01 1.58169 0.49392 1.69583 0.6241)7 1.02337 I11 -5.00722E-01 1.57S71 0.43104 0.86624 0.62249 1.024799
" " I S ' " ^ .^ S ^ T e- T I 1.57656 - C .39942 - I . 14964 0.625 71 1.02569113 -1.74694E-01 1.57 789 -0.61081 -0 .12257 0.63012 1.02625514 -1.32975E-01 1.57751 0.62821 0.07668 0.63148 1.02661515 -9.16022E-02 1.57 729 0.5972 6 0.69828 C . 63147 1.02684516 -5.73954E-02 1.5/716 0.56918 0.69880 0.63049 1.02699517 -3.74682E-02 1.57709 0.61534 0.71649 0.62458 1.02709118 -2 .38352£-02 1.57704 b .61231 0.73828 0.61438 1 .02715519 —1.47468E-02 1.57702 0.60395 0.74S81 0.59367
-3 .1 3 5 ? IE -02 EXTRAPOLATION WITH 2.0948 1.027285?0 3 .73554E-03 1.00000 -0 .24958 -1 .69596 1.77761 1 .C 2728521 1.91975E-03 1.57700 0.51583 0.58743 -0 .22573 1.02728222 1. 5192 OF- 0 3 1.57699 0. 79288 0.51586 0.84607 1.02728223 l . i % H 6f-'34 1.5*699 0. 4834 7 0.88053 1.04687 1.02728224 6.68526E-04 1.57699 0.91224 0.82188 0.99751 1.027 28225 4.0245 IE—04 1.57699 0.60240 0.82732 0.99494 1.02728226 2.4318 7E-04 1•57 659 0. 6045 1 0.90168 0.99329 1.02728227 1.64986C— 04 1.57699 0.67860 5. 7? 2<56 1.00415 1.027 28328 1.23024E-04 1.57699 0.74579 0.85892 1.00745 1 .027283I ’i 9.0599 IF -05 1.'576^9 0. Iibt>2 (i.851Cfl S .98619 1.027 283
END OF EIGENVALUE CALCULATION - ITERATION TIME 0.805 MINUTES
CONVE RGFNCE IVOICATION BY MINIMIZING THE SUM UF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 1.0000019 K 1.0272770
LEAKAGE 3. 45 31 IF 11 TOTAL LOSStS 6.40828E 12 IO IAL PRODUCTIONS 6.58312E 12 REACTOR POWERtHATTSI l.OOOOOE 03
GW3SS NEUTRON BALOTC'E---------------------------------------------------------------------------------------------------------------------------------------------------------------------------
CEP IFT LEAKAGE TOf< LFAkAGb Kl'l LfcTRAGfc BUI COKSTTE FN T LEAKAGE BAk T'EAkaTJE 8**2 LOSSES 1/V LOSS XENON LOSS 1 ? •45977E 10 2.45837F 10 0 .0 0 .0 8.68050E 08 7 .3U 10E 10 0 .0 0 .0 0 .0
~1 1 • 7431 OF 10 1.74216E 10 070 570 6.06f>42E Ob 5724l5lE~TG STC OTO OTO3 2.65618E 10 2.65486E 10 0 .0 O.C 9.41098E 08 8.02248E 10 O.C 0 .0 0 .0
SUM 6.65905E 10 6.85S39E 10 0 .0 0 .0 2.41569E 09 2.05751E 11 0 .0 0 .0 0 .0
grp— a &s o r p t i o n s — o u t - s c a t t e r ----------- souRct----------------------------------------------------------------------------------------------------------------i n - s c a t t e r — r c m n i K n — TCTAL GAIN'S--------------PRQD/ABSCRP1 0 .0 6 . 28515E 12 6.40827E 12 0.0 6.40830E 12 6.40827E 12 0 .0
"2---- r.U JW '/r ~T7.— 5 . l6 m fc 12— CFTD----------------- SVTS'JTFt- 12— 57ZS5T7^T2— 6.23515t 17-----------------------------------------------7.54925E-013 3.02695E 12 0 .0 0 .0 5.16124E 12 5.16122E 12 5 .1612 'E 12___ _________________________________ 1.15398E 00
SUM 6.06296E 12 1.14464F 13 6.40827E 12 1.14464E 13 1.78546E 13 1.78546E 13
END OF CASE - TOTAL CPU TIME WAS 0.88 MINUTES TOTAL CLOCK TIME HAS 2.74 MINUTES
200
201
3-0 <X,Y,Z ) BUCKLING SEARCH (OLD WHIRLAWAY CASE)9X9X5X2 GROUP. 810 POINTS STREAM OF CltftTION CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 - 2 0 1 0 0 0 0 0 1 1 0 0 0 0 01 0 * 0 0 1 0 0 0 1 0 0 i 0 0 0 0 0 a o 0 0 0 0 0
100 1 06 10 l.OOOOOOE 01
2 3 0 0 9.999999E-04
0 0 0 9.999999E 09
0 0 0 9.999999E
023
00 .0
0 0 0 5 6 8.999997E
12-02
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECT1UN 003
0 0 0 0 11 0 0 0 0 0 1 0 0 l .0 0 0 0 0 -1 0 0 0 09.999999E—05 1.000000E-05 9.999999E 29 0 .0
9.999999E-05 1 .OOOOOCF 01
9.999999El.OOOCOOE
-0500
9.999999E-05 U.O l.OOOOCOE 00 1.5999*9E 00
LEFT,TOP,RIGHT,BOTTOM,FRONT,BACK BOUNDARY CCNDITICNS ARE0 .0 9.999999E 29 9.999999E 29 6 .0 9.999999E 29 9.999999E 29
THftEE OlHENSIONAL SLAB GEOMETRY tX~,Y,Z> WTbTH 2.500000E 01 HElCHT f.800000E 01 DEPTH 1.50U0Q0E 01
Re g io n s p e c if ic a t io n s PTS REGION WIDTH
5 8.O0OO66E 00 5 &.0000&0E 00 3 9 . OOOOOOE 00
PT5 hfc'tlON Hf Ight 19 1.800000E 01
PTS REGION DEPTH 5 1t 500000E 01
~X -O H T . POI NT S--------9-----------------------7 -D If t . POINTS--------9-----------------------r -131R T'TO TOTS--------7
DISTANCES TO ffFSH- tNTERVAT" IN TfftFSC ES----------------------------------------------------------------
J D IST. 2 2.000 3 4. 000 4 6.000 5 8.0C0 6 12.000 7 16.000 a 19.U00 9 22.000 10 25.000
I DIST.2 2.000 3 4 . COO 4 6.000 5 8.000 b 10.000 I 12.000 8 14.000 9 16.000 10 18.000
KB DIST 2 3 .000 3 b.000 4 9.000 5 12.0G0 6 15.000
DISTANCES TO FLUX POINTS
J DIST.1 1.000 2 3.000 3 5.000 4 7.0 00 b 10.000 6 14.000 / 17.500 a 20. i>00 9 23.500
1 D'151. 1 1.000 2 3.000 3 5.000 4 7.000 5 9.000 6 11.000 7 13.000 a 15.000 9 17.000
KB 01 STT----- TT5C5------ 2-----S75!J<5------ 3----- FT57J(3------ T0.5OT------------5— 13.500
202
ZONE INPUT BY REGION
P L A N E NUMBER 11 1 1
ZONE NUMBER AT EACH MESH INTERVAL
SPECIFICATION FOR LAYER NUMBFR 1
1 2 3 4 5 6 7 8 9
1 1 1 1 1 1 1 1 1 12 1 1 1 1 1 1 1 1 13 1 1 1 . 1 1 1 1 1 14 T " 1 1 1 1 1 T " " l 15 1 1 1 1 1 1 1 1 16 I 1 1 1 1 1 1 1 17 1 1 1 I 1 1 I 1 18 1 1 1 1 1 1 1 1 19 1 1 1 1 1 i 1 1 1
SPECIFICATION FOR LAYER NUMBER 2
1 2 3 4 5 6 7 8 9
. 1 1 1 1 I 1 1 1 1 12 1 1 1 1 T 1 1 1 13 1 1 1 1 1 1 1 1 14 1 1 1 1 1 1 I " 1 15 1 1 1 1 1 1 t 1 16 T " 1 1 1 1 1 1 1 17 1 1 1 1 1 1 1 1 18 1 I I 1 1 1 1 1 19 1 1 1 1 1 1 1 1 1
SPEC7 FICATION FOR LAYER NUMBER 3
1 2 3 4 5 6 7 8 9
1 1 1 1 1 1 1 1 12 T i l 1 1 1 l l3 1 1 1 I 1 1 1 14 1 t 1 1 T5 1 1 1 1 16 1 1 1 1 1 l l l7 1 1 1 1 1 1 1 1S... 1 1 1 I" T " T T 19 1 1 1 1 1 1 1 1
SPECIFICATION FOR LAYER NUMBER 4
1 2 3 4 5 6 7 8 9
1 1 1 1 1 1 1 1 1 )i 1— i— i— i— i— i— i— i— r3 l l l l l l l l l
r ooUG
4 1 1 1 1 1 1 1 1 15 1 1 1 1 1 1 1 1 16 i i i i i i i i i7 i l l l l l l l i8 i i i i i i i i i9 l i i i i i i i i
SPECIFICATION FOR LAYER NUMBER 5
1 2 3 4 5 6 7 a s
1 1 1 1 1 1 1 l l l2 1 1 1 1 1 1 l i i3 1 1 1 1 1 1 l l i4 1 1 1 1 1 1 i l l5 1 1 1 1 1 1 l l l6 1 1 1 1 1 1 1 i t7 1 1 1 1 1 1 i l l8 I - y - 1 1 1 1 l l l9 l l 1 1 1 1 l l l
MESH OVERLAY INPUT
ZONF NUMBER 25 6 1 9 1 5
Z O NE n u m b f r t
7 9 1 9 1 5
ZONE NUMRER AT EACH MESH INTERVAL
SPECIFICATION FOR LAYFR NUMBER 1
1 2 3 4 5 6 7 B 9
I 1 1 1 1 2 2 3 3 32 1 1 1 1 2 2 3 3 33 1 1 1 1 2 2 3 3 34 1 1 1 1 2 2 3 3 35 1 1 1 I 2 2 3 3 36 1 1 1 1 2 2 3 3 37 1 ! 1 1 2 2 3 3 38 1 1 1 1 2 2 3 3 39 I 1 1 1 2 2 3 3 3
SPECIFICATION FOR LAYFR NUMBER 2
1 2 3 4 5 6 7 8 9
1 1 1 1 1 2 2 3 3 32 1 1 1 T 2 2 3 3 33 1 1 1 1 2 2 3 3 34 1 1 1 1 2 2 i 3 35 1 1 1 1 2 2 3 3 3
1 1 T 1 2 -2 3 3 37 1 1 1 1 2 2 3 3 38 1 1 1 1 2 2 3 3 39 1 1 1 I 2 2 3 3 3
SPECIFICATION FOR LAVER NUMBER 3
1 2 3 4 5 6 7 8 9
1 1 1 1 1 2 2 3 3 32 1 i i 1 2 2 3 3 33 1 l l 1 2 2 3 3 34 1 l l 1 2 2 3 3 35 , l l 1 2 2 3 3 36 1 l l 1 2 2 3 3 37 1 l i 1 2 2 3 3 3
1 1 1 1 t 2 4. 3 39 1 l l 1 2 2 3 3 3
S P E C IF IC A T IO N FOR LAYER NUMBER 4
1 2 3 «• 5 6 7 8 9
1 1 1 1 1 2 2 3 3 32 1 1 1 1 2 2 3 3 33 I 1 1 1 2 2 3 3 3T 1 1 1 1 2 2 5 35 1 1 1 1 2 2 3 3 36 1 1 1 1 2 2 3 4 37 1 1 1 1 2 2 3 3 36 1 1 i 1 2 2 3 3 39 1 1 1 1 2 2 3 3 3
S P E C IF IC A T IO N FOR LAYER NUMBER 5
1 2 3 4 5 6 7 8 9
1 1 1 1 1 2 2 3 3 32 1 1 L 1 2 ' 2 4 3 33 1 1 1 1 2 2 3 3 3 .
1 1 i 1 2 2 3 3 35 1 1 1 1 2 2 3 3 36 1 1 ' i r 2 2 3 3 3 •7 1 1 i i 2 2 3 3 38 1 1 i i 2 2 3 3 3“ ..................9 1 1 i i 2 2 3 3 3
F IS S IO N SOURCE D IS T R IB U T IO N AND SUM 1 .0 0 0 0 0 0 . 0 1 .0 0 0 0 0
PERTURBATION INPUT - SECTION 0*0o o 0 5 S o o 5 S 3 o 0 oTS o To o T c F
COR'E S1TTRAGE DIFFEREN CE' ( W ORDTTFQUfinUN CLIRSI AN IS 17'U IN STE AD OF STORfcD------------I3 F 6
f w ' n<m constattts tu u / B t stored in core---------------------------------------------------------------------------------------------------------------------------
RDRCER U f COLUMNS, ROWS;. PL ANS5» ' GROUPS, UPSCAT , dOrfNStAT* kEGlQNS, AND £aNES 5 9 5 2 0 1 5 3
HEH OR YTO CATIO W 5 R E S E R ? E TrF O trD * TA STORAGE-— OTCRff MEMORY LOCATIONS USED FOR T H IS PROBLEM----------------- 8262MEMORY LOCATIONS „ J T USED 31738
SO
cs
3-D ( X .V .Z ) BUCKLING SEARCH (OLD HHIRLAWAV CASE!9X9X5X2 GROUP, 810 POINTS STREAM OF CITATICN CASES ORNL 72
LINE RELAXATION WILL BE DONE CN ROMS .COLUMNS .AND PLM ES - 1 INNER IT E R A T IO N S■ i t t h i t r^< r ? A lu E 5 OF the SEARCH ^ACTOR FOR ABSORPTICN ANO TOTAL LOSS ARE —2 .75116E-01 -5 .49130E 01
ITERATION1 FLUX CHANGE BETA MU-1 MU-2 MU-3 K SEARCH FACTOR1 3.73.813E 00 1 .0 0 000 7.47626 -1 .9670/ 0 .0 0.066221 l.OOOOCD 002 1.10976E 00 1.88235 1.40664 0.01641 -0 .48320 0.045170 8.779910-013 3.54570E 00 1.78947 6.7407 0 0.01960 0.46375 0.053144 7.681830-014 3.68834E 00 1.72238 4.72857 0.03253 0.47602 0.055153 6.69355D—015 "OO 1.67696 1.73339 0.06271 0.58613 0.05 710 7 5 .8041 ID—016 1.32409E 00 1.64 755 2.29506 0.12985 0.61485 0.058744 5.003&0D—017 2.94818E 00 1.62905 5.17476 0.11482 0.64979 0,060149 4 . 28315D-018 1.71740E 00 1..61 762 2.29993 0.32965 0.66975 0.061315 2 .98634D-019 U45105E 00 1.61064 2.29596 0.06 624 0.66340 0.063141 V .114400-02
10 -3 .11387E-01 1.60641 -0 . 52598 0 .0 0.64175 0.066366 -1 .578440-01------- l r 2.B3885E-01 1 .60*8 * -0 .62779 -0 .6 '2 7 7 9 1 0.62278 0.070630 —2 .2009 10—0112 -1 .93981E-01 1.60231 -0 .87729 0 .0 0.76590 0.071913 -2 .200910-0113 -1 .80202E-01 1.60139 0.74876 0.74876 0.83252 0.071964 -2 .200910-0114 -1 .74023E-01 1.60083 0.79169 0.79169 0.83522 0.071971 -2 .888710-0115" -1 .67T906 -O l 1.60050 0.79639 0.79639 0.77146 0.073246 -3 .033150-0116 -1.54282E-01 1.60030 0.76521 0.76 521 0.83328 0 .073 56 7 -3 .184800-01
— i r ... .... ~ I T W 5 ? C r n i - 1 .6 0 0 18 0.81^24 0.81924 0.83550 0.073869 - 3 . 34404D—0118 -1 .4 5 1 89E-01 1.60011 0.82629 0.82629 0.83740 J . 074186 -3 .511240-0119 -1 .419286-01 1.60006 0.83562 0.83 562 0.83916 0.074521 -3 .6868 00-0120 - 1* 38671E-01 1.60004 0.83838 0.83838 0.84079 0.0748/5 -3 .671130-012 l 1.60002 0.84044 0.84044 0.84237
-8.24242E-01 EXTRAPOLATION WITH 5.2673 0.077434 -4 .267920-01kz -1 .1 8 3 0 0 6 -0 1 I.OOOCO 0.75600 0.75600 5.33289 0.57766 3 —4 . 26792D-0123 -3 .99681E-01 1.60001 2.97886 2.97886 0.02989 0.076410 -4.374610-01
~ 24 - l.d 2 0 4 a E -0 l 1 . 600nc 7 jr2¥845" ' 0 .0 0»b649b 0 .0 7 6 3 1 3 -4 .539990-0125 -1.42174E-01 1.60000 0.59813 0.59813 0.85848 0.076649 —4.940640—0126 -1.26O68E-01 1.606OO 0.76065 0. 76065 0.82424 0 .0 1/4b i -5 .187660-0127 -1.15768E-01 1.60000 0.80253 0.80253 0.84990 0.078029 -5 .447040-0128 - =T :0 '63F 5 t^n 1.60000 0 .8 1 2 5 7 ‘J . 81 i. 5 I 0.85023 0.078599 - 5 . >19390-1>129 -1.00897E-01 1.60000 0.84751 0.84751 0.84998 0.079 205 -6 .005360-01io -9 .53650E-02 1.6O0OO 0.84981 0 .8 4 9 fii 0.84922 0.079850 -6 .305620-0131 -8 .95324E-02 1.60000 0.84931 0.84931 0.84721
-5 ;S '4 Z'22e-6l EXTRAPOLATION WITH 5.6360 0.082526 -6.95193D—0132 -5n35833E-02 1.00000 0.54490 0.54490 5.78122 0.083078 -6.95193D-0133 " -2 .3 2 4 1 4 E -0 1 'll'ATJOTr 4.10502 4 .1 0 5C2" 0706344 0 . C8230 6 -7 .125730-0134 -1 .0 6 4 2 7E-01 1.60000 0.35149 0 .0 0.88514 0.C82 502 -7 .664500-01S5 -8 .2 7 5 7 5 E -0 2 1.60000 0.69484 0.694fl4 0.77222 0.083 772 —8.0477 ID-0136 -5.85892E-02 1.60000 0.64937 0.64S37 0.79865 0,084740 - 8 . 45005D-0157 -4 .6 7 5 O 5 E -0 2 1.60000 0.75119 0.75119 0.76516 0.085 76 7 - 8 . 87259D-0138 -3 .80051E-02 1.60000 0.77493 0.77493 0.70883 0.086869 -9 .316210-0139 — 2 . 8/6 6E —02 1.60000 1.85497 0. 60072 0.088054 -9 .782620-0140 2.34814E-02 1.60000 - 0 . 79276 -1 .34930 0.33324 0.089329 -1.0064C0 0041 1.922616-02 1.6000O 0.83801 0.52400 -0 .21144 0.090139 -1 .000590 OC42 8 . 84724E-03 1.60000 0.46902 0.65389 0.03666 0.090017 -9 .998750-0143 2.53677E-03 1.60000 0.28927 0.25799 -1.26431 0.089997 -1.00001D 0044 9.83238E-04 1.60000 0.38858 0.47483 0.08640 0.090000 - 1.0000 10 UO45 -6 .6 & 2 2 6 6 -0 4 1.60000 -0.6B:\29 —0 . 65544 0 .0 8 6 4 9 O.09O000 -l.O o O O c o 0046 -8.20816E-C4 1.60000 1.22753 0.47032 -2 .42622 0.090000 -9 .999960-014 t ‘ ' 2.8896 3E-04 1.6001)0 - 0 . 35176 -0 .29174 1.60331 O.09OUOO —9.999950—0148 -4.15444E-0S 1.60000 -0.14331 -0 .37236 0.88381 0.090000 -9 .999900-01
CONVERGENCE INDICATION BV MINIMIZING THE SUK1 OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 1.0000019 K 0.0899997
END OF CR 5?IC fttITV SEARCH - ITERATION TIME 0.131 MINUTES
BUCKLINGS MULTIPLIED 8V -9 .99990E -01 , FRACTION ABSORPTIONS IN SEARCH PARAMETER -0 .266016
iE M £ ^ _ A v 2 5 7 5 7 E 19 TOTAL LOSSES 1.01092E 19 TOTAL PRODUCTIONS 9.09827E 17 REACTOR POwERIWATTS). l.OOOOOE 07
ADJOINT PROBLEM FOLLOWSITERATION FLUX CHANGE beta MU-1 MU-2 MU-3 K
1 4.87929E 30 l .0 0 0 0 0 * * * * * * * * * * -0 .2 8 6 8 * 0 .0 0.090000? 2.95952E 01 1.8823b 29.59515 3.24146 0 .0 0.0900003 2 .41423E 00 1.78947 2.49580 0.73649 0 .0 0.0900004 2.99386E 00 1.72238 4.23395 0.092C6 0 .0 0.0900005 1.77001E 00 1.67696 2.37190 0.26755 0 .0 0.0900006 5.71321F-01 1.64 755 0. a926 5 0.43337 0 .0 0.0900007 - 5.12162E-01 1.62905 -1 .40861 -0 .57359 0 .0 0.0900008 4.07093E-01 1.61762 -0 .38776 -0 .80105 0 .0 0.0900009 6.21300E-02 1 .6 1 0 6 4 0.2147 5 0. 192S5 0 .0 0.090000
10 2 .2 2 1 8 / e - o 2 1. 606*i 1 0.3?984 0 .2 1 9 2 b 0 ,0 0.09000011 1.29766E-02 1.60365 0*59702 0.27070 0 .0 0 . 090£>0012 - 1. 8922 IE -0 3 1.60231 -0 .14771 -0 .07065 0 .0 0.09000013 1.09673E-04 1.60139 -0 .05785 -0 .26569 0 .0 0.09000014 3 .6?396E— 5 1.60083 0.3304? 0 .229*6 0 .0 0.090000
fcNCl OH AUJC1IN1 CALCULATION - I ItK ATlON TIME 0.034 MINUTES
CONVERGENCE i n d i c a t i o n BV MINIMIZING THE SUM OF THE SQUARES OF The RES I CUES - RELATIVE AbSOR TION 0*9999553 K 0»0900005
GROSS NEUTRON BALANCE
GrP1
LPT '..FAKAGE 0 .0
TOP TEaKAGE " 1.77426E 18
"RTT CEAKUGF" 2.04650E 17
BOT LEAKAGE 0 .0
FTJT LEAKAGE 4.9564BE 18
BAK LEAKAGE 4.95649E 18
0**2 LOSSES -2 .54697E 18
l/V LOSS 0 .0
XENON LOSS 0 .0
2 0 .0 9 .90U1V£ 16 j . 1101 3b 16 0.0 2 . 'f6 W lE IV 2.76792E 1/ -1 .42233E 1/ 0 .0 0 .0
SUM rt.o 1.87T37E Iti 2.7571.1 F 1 I 0 .0 5.53327E 18 5.23329E 18 -2 .68920E Id 0 .0 0 .0
GRP ABSORPTIONS OUT-SCATTER SOURCE IN-SCATTER TOTAL LOSSES TOTAL GAINS PRGD/ABSCRP12
1.57100E 176.56374E 16
6.0717BE 170 .0
1 .Ol092E 0 .0
iy o .d6.0717 5E 17
1.01092E 19 6.07170E 17
1.01092E 19 6.07175E 17
2.75328E 00 7.27159E 00
SLiM 2.22737E 17 6.07175E 17 1.01092E 19 6.07175E 17 1.07164E 19 1.07164E 19
AVERAGE FLUXFS BY ZONE AND GROUP
ZONE 1— CORE ZONE 14. 82498E 16 2 . 77184E 15
ZONF1.
2— CUKI - ZUNE 2 81258E 16 1.85364E 15
ZONE 3— AXIAL BLKT 13. 66449E 15 6. 313 49E 14
ZONE4.
AVERAGE POWER 07559E 03 5 .
DENSITIES!W A T T S / C C ) 540loF 0? 0 .0
3-D tX ,V ,Z > BUCKLING SEARCH (ULD WHIRLAMAY CASEt_____________________________9X9X5X2 GROUP, 810 POINTS STREAM OF CITATION CASES UKNL 72
PtftTiJftBATIBKi HESJl TS— DELtA-K/IK*O^LTA-S> WH^RE $ REPRESENTS MACRC. CROSS SECTIONS. LAMbOAIPHl* H PH I) = j . 92425dE Ci>
COMP1
NAME CORE ZONE 1
GRP1
SIGA,SlGR»DB**2 NU*S1GF - I.IC 4 5 6 0 E 01 1.227289E 02
OIFF. COEF. —5.92275IE—01
B*#2—1.656841E 01
2 CORE ZONE 221
-6 .*21769E 00 7.000949E 00 -2.113914E 00 2.348793E 01
—3 .475089E—01 —1.44S156E—01
—8.066121E 00 - 3 . 593654E 00
3 AXIAL BLKT 1i1
-1.96271BE 00 2.345219E 00 -1.872991E-01 2 .081100E 00
-1.184266E—01 -2.000O47E-02
—2.217869E 00 - 2 . 247588E—01
2 —1.937637E—01 3.451864E-01 -1.991225E-02 —1.68591BE—01
COMP1
NAME CORE ZONE 1
GRP.1
K ------ 5IGSIFR0H ALL GRP5. KK TO1 .104560E 01 6.300853E-01
GRP. K)
2 CORE ZfV'E ?21
17T7ff7ff8E 52 6.721764E 00 2.113914E 00 2.110696E-01
3 AXIAL BLKT 121
1.477719E 01 1.962718E 00 1.872991E-01 3.10667BE-02
2 1.175W E 00" 1.937337E-01" "
EhD OF CASE - TOTAL CPU TIME Ua 5 0.22 MINUTES TCT/T CLCCK TIME WAS 1.45 MINUTES
JOB WAS RUN ON 03-11-72 CN THE IdM 360/SI
3 -D , 90 DEGREE ROTATIONAL SYMMETRY, QUARTER SECTICN WITH BLACK ABSORBER9X9X3X2 GROUP, 486 POINTS STREAM OF CITATION CASES ORNL 72
GENERAL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 c 0 0 1 0 0 0 0 0 0 1 0 0 0 0 01 0 1 1 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
100 100 10 2 3 0 0 1.50000CE 00 9.999998E-03
0 0 9.999999E
009
09.
0 0 0 9999S9E 23
00. 0
0 0 01
12 6 .OOOOOOE
1200
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 n 11 0 0 0 0 0 0 0 2 C 1 1 1 0 0 0 0 0 0 09.999999E-05 9.999999E-05 9.999996E-02 0 .0
9.999999E—05 2.500000E-01
9.9999S9E-05 9 .5000C0E-01
9.999999E—05 0 .0 2.500U00E—01 0 .0
LEFT, TDP, RIGHT, BOTTOM, FPCINT, BACK BOUNDARY CCNDITICNS ARE9.99$$96F-02 9 .^ 9 9 9 o£-02 RUTATIQN(90> R0TATICNI90I 0 .0 0 .0
ROC flHO- CONST ATJTT OTT ALL GROUPS IN — I— T5— 4.6<52006E-01--------------------------------------------------------------------------------------------------------------------------------------------
THRFE DIMENSIONAL SLAB GEOMETRY (X .Y ,Z ) WlbTH 3.GOOOOOE 01 HEIGHT 3 .OOOOOOE 01 DEPTH 9.999999E-01ro------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- 0vo
REG 1 UN SPECIHCATTUKTS----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------PTS REGION WIDTH
3 9 .OOOOOOE 00 3 1.200000E 01 3 9.COOOOOE 00
— p t s R E G io h i 'f lr r c m --------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------3 9 .OOOOOOE 00 3 1.200000E 01 3 9.C0U000E 00 _____
PTS REGION DEPTH3 1 .OOOOOOE 00
X -D If t . POINTS------- 9-----------------------Y - IM R . POINTS-------9----------------------- Z - D I k . POINTS--------J
DISTANCES T(J HbSH ’IN IERVAL I Nl bKf-AlbS
J B IST. 2 3.000 3 6.000 4 9.000 5 13.000 6 17.000 7 21.000 8 24.000 9 27.000 10 30.000
I DIST.2 3.000 3 6.000 4 9.000 13.0C0 0 17.000 t 21.000 a 24.000 9 27.000 10 30.000
KB pi ST 2 0.333 3 0.667 4 1.000
DISTANCES TO FLUX POINTS
J OIST.1 1.500 2 4.500 3 7.500 4 1 1 .COO 5 15.000 6 19.000 7 22.500 B 25.500 9 28.500
T T ilS T . 1 1.500 2 4. 500 3 7.500 4 12.000 5 15.000 6 19.000 7 22.500 8 25.500 9 28.500
KB 01 STT 57167 2 0.500 3 0.833
TONE 1NPUT~BY REtilfiN--------------------------
PLANE NUMBER 11 2 3____________________________2 2 33 2 1____________________________
ZONE NUMBER AT EACH MESH INTERVAL
SPEC! FICATION FOR LAYER NUMBER 1
1 2 3 4 5 6 7 8 9
1 1 1 1 2 2 2 3 3 32 1 1 1 2 2 2 3 3 33 1 1 1 2 2 2 3 3 34 2 2 2 C 2 J •J 3 35 2 2 2 2 2 2 3 3 36 2 2 2 2 2 2 3 3 37 3 3 3 2 2 2 1 1 18 i i 4 £ 2 2 1 1 19 3 3 3 2 2 2 1 1 1
S P E C IF IC A T IO N FOR LAYER NUMBER 2
1 2 3 4 5 6 7 8 9
1 1 1 1 2 2 2 3 3 32 1 i i £ 2 2 3 3 ■»3 1 l l 2 2 2 3 3 34 2 2 2‘ 2 n 2 3 3 35 2 2 2 2 2 2 3 3 36 2 2 2 2 2 2 3 3 37 3 3 3 2 2 2 1 1 1
3 3 3 2 2 2 i 1 I9 3 3 3 2 2 2 I 1 I
SPECIFICATION FOR LAYER NUMBER 3
1 2 3 4 5 6 7 8 9
1 1 1 1 2 2 2 3 3 32 1 1 I 2 2 2 3 3 33 1 1 1 2 2 2 3 3 34 2 £ 2 2 2 2 3 3 35 2 2 2 2 2 2 3 3 36 2 2 2 2 2 2 !4 3 37 3 3 3 2 2 2 1 1 1B 3 3 3 2 2 2 1 1 19 3 3 3 2 2 2 I 1 1
FISSION SOURCE DISTRIBUTION AND SUM 1.00000 0 .0 1.00000
roHO
CORE STORAGE DIFFERENCE ( WORDS) EQUATION CONSTANTS I/O INSTEAD OF STORED 864
EOUATION CONSTANTS WILL RE STOREO IN CORE
NUMBER OF---- COLUMNS , POHS, PLANES, GROUPS, UPSCAT, DOWNSCAT, REGIONS, AND ZONES 9 9 3 2 0 i 9 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE---- 4000QMEMORY LOCATIONS USED FOR THIS PROBLEM----------- 6096MEMORY LOCATIONS NOT USED-------------------------------- 33904
ZONE MACROSCOPIC CROSS SECTIONS
ZONE NAME GRP D SIGR SIGA NUSIGF BSQ POHER/FLUX1 CBr E zonS 1 1
20 .0C.O
0 .00 .0
0 .00 .0
0 .00 .0
0 .00 .0
0 .00 .0
2 CORE ZONE 2 1 1.70000E 00 5.20000E-03 7. OOOOOE—04 1.0QOOOE-O3 0 .0 5.00000E—152 1.13000E 00 0 .0 6.30000E-03 2 . 50000E-02 0 .0 2.50000E-13
3 Ex'IAL "BUT 1 12
1 .2OOO0t 00 8.70000E-01
6.70000£—03 0 .0
5.2600<5g-04 8 .00000E-03
0 .00 .0
0 .00 .0
0 .00 .0
SCATTERING MATRIX
ZONE GRP TO GRP 1 2- j - - y ■ 0 . 0 0 . 0
2 0 . 0 0 . 0
2 1 0 . 0 5 .2 0 0 0 0 E -0 32 0 . 0
O•o
0 . 0 6 .7 0 0 0 0 E - 0 3 ’2 0 . 0 n . n
211
3 -0 , 90 DEGREE ROTATIONAL SYMMETRY, QUARTER SECT ICN WITH BLACK ABSORBER9X9X3X2 GROUP, 486 POINTS STREAM OF CITATION CASES ORNL 72
LINE RELAXATION WILL RE DONE ON ROWS - 3 INNER ITERATIONS!ITERATION FLU* CriANliE BETA MU-1 MU-2 MU-3 K
1 -4.40549E-02 1.00000 -0.08811 0.01298 0 .0 0.37816O2 -2.07959E-01 1.80966 4.51250 15.60664 -0 .03733 0.3913533 -2.02187E-01 1.68019 0.77006 1.07649 1.11314 0.4015154 -1.24678E-01 1.60222 0.49197 0.73692 0.66166 0.404J.755 -7 .7378 IE-02 1.55866 0.54324 0.70501 0.73304 0.4044266 -6 .17429£-02 1.53534 0.73619 0.81991 0.85299 0.4038847 -5.28412E-02 1.52314 0.80299 0.37304 0.90216 0.402816a -4 .70120E-02 1.51684 0.84267 0.90112 0.92792 Q .4013509 - 4 . 26070E-02 1.51360 0.86369 0.91252 0.94088 0.399564
10 —3.90391E—02 1.51194 0.87722 0.918Q3 0.94809 0.39751911 -3.60072E-02 1.51109 0.B863 3 0.920S4 0.95235 0.39526212 -3 .33886E-02 1.51066 0.89389 0.92276 0.95510 0.39283813 - 3 . 10795E-02 1.51044 0.89976 0.92367 0.95682 0.39028114 -2.90226E-02 1.51033 0.90480 0.92480 0.95823
-3.20913E-01 EXTRAPOLATION WITH 10.7365 0.35643115 -6 .7 3 0 9 lt -0 3 1.00000 0.22519 0.41352 10.93651 0.35514816 -1.24463E-02 1.51024 1.83668 1.78738 0.03973 0.35242217 -1 .2 7 il£ E -6 2 i-51"525 1.00860 0.99436 1.16432 0.34933018 -1.22864E-02 1.51022 0.95427 0.93162 0.98348 0.34637219 -1.17549E-02 1.51021 0.94498 0.92287 0.97405 T ).3-4355720 —1 .12848E-02 1.51021 0.94872 0.93449 0.97392 0.34087021 —1.08676E-02 1.51021 0.95216 0.93802 0.97331 0.33829822 -1 .0 4 8 1 4E-02 1.51021 0.95398 0.93910 0.97256 0.33583423 -1.01221E—02 1.51621 0.45566 0.94340 0.97203 0.33346824 -9 .78196E-03 1.51021 0.95661 0.94647 0.97168 0.33119425 - ‘>.466206-03 1.51021 0.95846 0.44641 0.97112
-1.95700E-01 EXTRAPOLATION WITH 20.4736 0.28341826 -5 .61676E-53 1.00000 0.60874 0.18812 20.61660 0.28323627 -1.00569E-02 1.51021 1.71828 1.64192 0.01487 0.28283228 -9.74119E—03 1.51021 ~»:9?a&7' 0.9B198 1.14274 0.28234529 - 8 . 80408E-03 1.51021 0. 8950 0 0.91891 0.96272 0.28185330 - 7 . 84916E-03 1.51021 0.88369 0.92135 0.95573 0.28136431 -7.03883E-03 1.51021 0.88972 0.94558 0.95755 0.28087832 -6 .34 I70E -03 1.51021 0.89462 0.95014 0.95822 0.28039833 - 5 . 73742E-03 1.51021 0.89898 0.95644 0.95920 0.27992534 -5.21541E—03 1.51621 0.90380 0.94951 0.96010 0.27945935 -4 .763195-03 1.51021 0.90853 0.95754 0.96124 0.27900136 -4.36890E-03 “ 1 .5 lo 2 i 0.91285 0.95025 0.96142 0.27855237 -4.02355E-03 1.51021 0.91693 0.96410 0.96208 0.2781133d -3.724106-03 1.51021 0.92185 0 .9 8 4 tO 0.96296 0.27768339 -3 .45618E-03 1.51021 0. '460 0.98441 0.96361 0.2772634o - ’l^OOSE-^S 1.51021 6.9 445 6.49303 0.96366 0.27685341 -3 .01367E-03 1.51021 0.93290 0.98897 0.96411 0.27645342 - 2 . 82848E-03 1.51021 0.93572 0.99488 0.96450 0 .2761)6443 - 2 . 66314E-03 1.51021 0.93888 0.98568 0 .96499 0.27568544 - 2 . 514B4E—63 1.51621 0.94180 0.98C27 0.96493 0.27531645 -2.37876E-03 1.51021 0.94351 0.97348 0.96532 0.27495746 =2.25741E-'03 1.51021 0. 94673 0.98136 0.96:180 0.2 745S847 - 2 * 14660E-03 1.51021 0. 94877 0.97985 0.96525 0.27426948 -2.O4S31E-03 "1.51021' 0.94984 0.97373 (T.'96665 0.27394049 -1.95044E—03 1.51021 0.95260 0.97180 0.96607 0.27362150 -1.86670E-03 1.51021 0;95520 0.96612 0.96603 '“ 0,27331151 -1 .78486E-03 1.51021 0.95437 0.96733 0.96716 0.27301052 -1. fll2 5 b -U 3 l .d lU Z l U.« /US u. U.2/^71453 -1 .64390E-03 1.51021 0.95900 0.96269 0.96573 0.272435
■ 54 -T.57970E-U3 1.51UZ1 0.9593 7 O.V720f 0 .9 6 170 ' 0.27215155 -1 .5193 8E-03 1.51021 0.96030 0.95577 0.96708 0.27189556 - 1 .46085E-03 1.51021 0.96002 0.97420 0.96633 0.271637 I5 7____ - 1 .40 5 8 9 E -0 3___ 1 .5 1021 0 .96C98____0 .9 6 743 _0 .96764_______ 0.27138b|
rolo
58 -1 . 3 5 7 0 2 E - 0 3 1.51021 0 .9 6 3 8 8 0 .9 6 4 7 1 0 .9 6 7 8 3 0 .2 7 1 1 4 659 - 1 . 3 0 9 0 4 E - 0 3 1.51021 0. 96333 0 .9 6 3 3 5 0 .9 6 6 0 6
-3 .4 4 3 4 1 E - 0 2 EXTRAPOLATION WITH 2 6 .2 7 8 6 0 .2 6 4 7 2 560 - 1 . 5 7 0 5 8 E - 0 4 1 .0 0 0 0 0 0.11982 0 .1 3 7 8 9 2 6 .3 1 9 2 t 0 .2 6 4 7 1 361 -1 . 9 9 1 3 9 E - 0 4 1 .51021 1 .26773 1 .1 5 8 6 3 0.0 0 3 5 9 0 .2 6 4 6 8 662 - J . 9 7 2 3 2 E - 0 4 1.51021 0 .99022 0 .9 6 8 5 1 1 .16380 0 .2 6 4 6 5 6 '63 - 1 . 8 1 6 7 5 E - 0 4 1.51621 0.9 2 0 9 4 0 .8 3 ^ 0 3 0.9 9 3 6 8 0 .2 6 4 6 2 764 - 1 . 7 1 6 6 1 E - 0 4 1.51021 0.94471 0 .9 3 5 1 3 0 .9 7 5 0 4 0 .2 6 4 6 0 065 - 1 . 6 7 4 2 9 E - 0 4 1.51021 0.9 7 5 1 8 0 .8 8 8 9 5 0 .9 8 1 1 6 0 .2 6 4 5 7 466 -1 . 5 6 4 0 3 E - 0 4 1.51021 0 .9 3 3 9 8 0 .8 7 5 0 5 0 .9 8 1 8 4 0 .2 6 4 5 4 967 -1 • 5 4 0 1 8 E -0 4 1.51021 0 .9 8 4 6 0 0 .9 1 0 7 6 0 .9 7 7 3 3 0 .2 6 4 5 2 568 - 1 . 4 9 3 6 9 E - 0 4 1.51021 0 .9 6 9 6 6 0 .9 4 1 2 2 0.9 8 3 0 6 0.2 6 4 5 0 3
' 69 -1 .4 5 5 5 5 f c -0 4 1.51621 6.47452 6.61254 0.9 8 3 5 5 0.2 6 4 4 8 170 - 1 . 4 0 6 0 7 E - 0 4 1.51021 0 .9 6 5 8 7 0 .9 4 8 7 5 0 .9 7 3 4 6 0 .2 6 4 4 6 0
" ?1 -1 . 3 2 7 9 9 E - 0 4 1.51021 0 .9 4 4 3 4 0 .7 8 3 8 1 0 .9 7 8 0 9 0.2 6 4 4 4 072 - 1 . 2 8 7 4 6 E - 0 4 1.51021 0.9 6 9 3 5 1 .0 3 4 5 1 0.9 8 0 5 3 0 .2 6 4 4 2 073 - 1 . 3 0 9 5 1 E - 0 4 1.51021 1 .0 1 7 0 0 0 .8 3 3 3 6 0 .9 6 9 9 6 0 .2 6 4 4 0 274 - 1 . 2 2 4 2 8 E - 0 4 1.51021 0 .9 3 4 7 9 0.8 B 0 02 0 .9 8 2 9 0 0 .2 6 4 3 8 475 - 1 . 1 9 9 2 5 E - 0 4 1.51021 6.9 7 9 4 3 0 .9 5 4 5 ? 0 .9 7 9 2 0 0.2 6 4 3 6 776 -1 . 1 4 5 0 1 E - 0 4 1.51021 0 .9 5 4 6 6 0 .9 0 4 7 8 0 .9 8 9 7 1 0.2 6 4 3 5 077 - 1 . 1 4 2 6 2 E - 0 4 1 .5 lo2 i 0.9 9 7 8 0 0 .6 3 1 5 9 0.9 7 8 0 0 0.2 6 4 3 3 378 - 1 . 0 9 0 7 6 E - 0 4 1.51021 0.9 5 4 5 1 1 .0 0 0 0 1 0.9 7 5 0 7 0 .2 6 4 3 1 879 -1 . 0 3 7 1 2 E - 0 4 1.51021 0.9 5 0 7 2 0 .7 5 0 01 0 .9 7 9 3 9 0 .2 6 4 3 0 380 - 1 . 0 1 8 0 5 E - 0 4 1.51021 0.98151 0 .4 4 4 4 5 0 .9 7 7 5 8 0 .2 6 4 2 8 981 -1 . 0 1 7 4 5 E - 0 4 1.51621 0 .9 ^ 3 1 l.oooO d 0.97732 0 .2 6 4 2 7 582 -1 . 0 0 0 7 6 E - 0 4 1.51021 0 .9 8 3 5 0 0 .7 5 0 0 0 0.9 7 5 6 9 0 .2 6 4 2 6 283 - 9 . 7 8 1 1 2 E - 0 5 1.5)021 0 .9 7 7 2 7 0 .0 6 6 6 7 0.9 8 1 3 9 0 .2 6 4 2 4 9
END OF EIGENVALUE CALCULATION - IT E R A T IO N TIM E 0 .1 7 3 Mi n u t e s
CONVERGENCE IN D ICA TIO N BY M IN IM IZIN G IHb SUM OF THE SQUARES OF THE r e s i cues - REl ATIvE XbS o r p t i o n 0 . 99 6 66 2 2 k 0 .2 6 4 3 7 8 4
LEAKAGE 6.57B40E 15 TOTAL LOSSES 2 .6 5 7 7 9 E 16 TOTAL PRODUCTIONS 7 .02 3 1 9 E 15 REACTOR POHERtWATTS) 2 .6 3 1 5 8 E 05
ADJOINT PROBLEM FOLLOWSITE R A T IO N FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 4.57711E 2d x• o o o o o * * * * * * * * * * - 0 . 0 1 9 6 8 0.0 0 .2 6 4 2 4 92 8.03612E 01 1.80966 8 0 .3 6 1 1 8 4 .6 0 3 3 3 0 .0 0 .2 6 4 2 4 93 2*96468E 01 1.68019 T T 5 . 01575 0 .9 3 5 6 3 0.0 0 .2 6 4 2 4 94 5.65157E 00 1.60222 5 .8 4 2 2 0 0 .6 8 8 1 5 0.0 0.2 6 4 2 4 95 2 .02722E 00 1 .5 5 8 6 6 " 2 .3 6 5 9 2 0 .7 1 4 T I " 0.0 0 .2 6 4 2 4 96 1.10932E 00 1.5 3 5 3 4 1 .6 5 6 5 4 0 .8 3 4 9 1 0.0 0 .2 6 4 2 4 9i 7.194o9E-0l 1.5 2 3 1 4 1.36792 O .S8T3tt 0.0 0 .2 6 4 2 4 98 5 .1 7 6 2 7 E -0 1 1 .5 1 6 8 4 1 .2 3 7 1 4 0 .9 1 8 6 3 0.0 0.2 6 4 2 4 99 3 .9 8 2 9 7 E -0 1 1.5 1 3 6 0 1.1 6 7 7 6 0 .9 3 2 6 2 0.0 0.2 6 4 2 4 9
10 3 .2 0 4 7 6 E -0 1 1 .5 1 1 9 4 1.1 2 5 0 9 0 .9 4 2 6 4 0.0 0 .2 6 4 2 4 9U 2 .6 5 9 6 9 E -0 1 1 .51109 1 .0 9 5 8 9 0 .9 4 7 5 8 0.0 0 .2 6 4 2 4 912 2 .2 5 6 9 4 E -0 1 1.5 1 0 6 6 1.0 7 4 2 6 0 .9 4 9 2 2 0 . 0 0.2 6 4 2 4 9u 1 .9 4 7 7 9 E -6 1 1 .5 1 0 4 4 1. 05 fBO 0 .9 5 0 9 2 u.o 0 .2 6 4 2 4 914 1 .7 0 2 9 2 E -0 1 1 .51033 1.0445 7 0 .9 5 2 8 0 0 . 0 0 .2 6 4 2 4 915 1 .5 0 4 7 2 E -0 1 1.5 1 0 2 7 1.6 3 4 0 6 0 .9 5 2 ^ 5 ” 0 . 0 0 .2 6 4 2 4 916 1 .3 4 0 9 5 E -0 1 1 .5 1 0 2 4 1.C2526 0 .9 5 3 7 4 0 . 0 0 .2 6 4 2 4 917 1 .2 6 3 7 1 E -0 1 1.5 1023 1 . 011)02 0 .9 5 3 3 0 0 . 0 0 .2 6 4 2 4 918 1 .0 8 7 0 0 E -0 1 1.51022 1 .0 1 1 7 4 0 .9 5 4 0 3 0 . 0 0 .2 6 4 2 4 919 9.86824fe-02 1.5 1021 i.od&53 0 .9 5 4 3 8 6 . 0 . 0 .2 6 4 2 4 920 8 .9 9 9 2 5 E-0 2 1.51021 1 .00193 0 .9 5 4 4 1 0 . 0 0 .2 6 4 2 4 921 ' 8 .2 3 9 8 4 E -0 2 r i s r f l s i 0 .99361 ' 0 .9 5 5 4 1 0 . 0 0 .2 6 4 2 4 922 7 .5 7 0 7 4 E -0 2 1 .51021 0 .9 9 4 5 0 0 .9 5 5 6 9 0 . 0 0 .2 6 4 2 4 923 6 .9 7 7 1 8 E -0 2 ' r : 5 i 0 2 i — 0799T37 0 .9 5 5 7 5 0 . 0 0 .2 6 4 2 4 924 6 . 4 4846E-02 1.5 1021 0.9 8871 0 .9 5 6 2 9 0 . 0 0 .2 6 4 2 4 925 5 .9 7 3 8 2 E -0 2 1.5 1021 T J .9 8 3 T 3 0 .9 5 7 5 2 0 . 0
1 .9 4 4 3 IE 00 EXTRAPOLATION WITH 3 4 .4 9 1 4 0 .2 6 4 2 4 926 - 6 . 19984E-03 1 .0 0 0 0 0 - 0 . 1 0 9 9 8 - 0 . 4 5 4 8 5 0 .0 0 .2 6 4 2 4 927 - 1 . 13243E-02 1.5 1021 1 .8 1 5 2 3 1 .7 4 3 1 7 0 . 0 0 .2 6 4 2 4 928 - 1 . 1 4 4 4 3 E - 0 2 1 .51021 0.9 9 9 1 5 1 .0 1 0 5 2 0 . 0 0 .2 6 4 2 4 929 - 1 . 0 9 5 0 3 E - 0 2 1.51021 0 .9 4 5 8 8 0 .9 5 8 4 5 0 . 0 0 .2 6 4 2 4 9
213
30 - 1 . 0 3 3 4 7 E - 0 2 1.51021 0 .9 3 3 4 5 0 .9 4 5 1 5 0 . 0 0 .2 6 4 2 4 931 —9 .7 5 8 5 3 E -0 3 1.5 1021 0 .9 3 4 4 9 0 . 94893 0 . 0 0 .2 6 4 2 4 932 - 9 . 22173E-03 1.5 1021 0 .9 3 5 7 7 0 .9 4 8 7 4 0 . 0
-1 . 5 1 8 7 0 E -0 1 EXTRAPOLATION WITH 1 6 .3 1 7 9 0 .2 6 4 2 4 933 -5 * 4 1 7 7 0 E -0 3 1 .0 0 0 0 0 0 .5 8 2 0 8 0 .2 8 4 8 9 0 . 0 0 .2 6 4 2 4 934 -9 . 7 7 5 1 6 E - 0 3 1.5 1021 1. 79452 1 .7 4 9 4 9 0 .0 0 .2 6 4 2 4 9
- 9 . t 5 8 8 3 E - 0 3 1.51021 0 .9 8 8 5 7 0. 95 802 0 . 0 0 .2 6 4 2 4 936 -9 . 3 0 3 9 3 E - C 3 1.5 1021 0 .9 4 4 0 8 0 .8 9 3 0 1 0 . 0 0 .2 6 4 2 4 937 -8 . 7 5 5 0 3 E - 0 3 1.5 1021 0.9 3 2 2 5 0 .8 7 9 2 4 0 . 0 0 .2 6 4 2 4 V3a - 8 . 2 2 6 0 4 E - 0 3 1.51021 0 .9 3 1 3 5 0 .8 7 575 0 .0 0 .2 6 4 2 4 939 -7 .7 2 6 0 1 E - 0 3 1.51021 0 . 9 3 1 4 9 0 .8 7 5 3 5 0 . 0 0 . 2 6 4 2 4 94 0 - 7 . 2 5 5 3 8 E - 0 3 1.51021 0 .93183 0 .8 6 9 4 9 0 . 0 0 .2 6 4 2 4 94 l — 6 . 8103 ? E -0 3 1 .5 1 o 2 l 0 .9 3 1 8 5 0 .8 7 4 3 6 0 .0 0 .2 6 4 2 4 942 -6 . 3 9 2 2 4 E - 0 3 1.51021 0.93221 0 .8 9 5 1 5 0 .0 0 .2 6 4 2 4 943 - 6 . 0 0 2 3 7 E - 0 3 1.51021 0 . 93301 0 .9 3 7 5 5 0 .0 0 .2 6 4 2 4 944 -5 . 6 3 6 2 2 E - 0 3 1.5 1021 0 .93336 0 .9 3 2 2 7 0 .0 0 ,2 6 4 2 4 945 - 5 . 2 9 1 2 8 E - 0 3 1.51021 0.93351 0 .9 3 3 9 3 0 .0
- 7 . 4 9 2 3 6 E - 0 2 EXTRAPOLATION WITH 1 4.0870 0 .2 6 4 2 4 946 -4 .3 9 4 0 5 E - 0 4 1 . 0 0 0 0 0 0.0 3 2 6 0 0 .3 5 1 0 0 0 . 0 0 .2 6 4 2 4 947 - 7 . 84218E-04 1.51021 1.7 8 3 9 4 1 .6 4 7 4 1 0 . 0 0 .2 6 4 2 4 948 - 7 . 7 4 4 4 3 E - 0 4 1.51021 0 .9 8 6 7 6 0 .9 8 4 3 0 0 . 0 0 .2 6 4 2 4 949 - 7 .2 0 0 8 4 E -0 4 1.51021 0 . 92909 0 . 95104 0 . 0 0 .2 6 4 2 4 950 - 6 . 6 5 9 6 3 E - 9 4 1.51021 0.9 2 4 1 7 0 .9 3 6 8 8 0 .0 0 .2 6 4 2 4 951 -6 .1 6 4 3 1 »= -G 4 1.51021 0.92501 0 .9 4 9 0 0 0 . 0 0 .2 6 4 2 4 952 -£ > .?345fc£- 04 1.51021 0.92971 0 .9 4 4 0 2 0 . 0 0 .2 6 4 2 4 953 - 5 . 2 9 7 0 6 E - 0 4 1.51021 0 .9 2 3 1 8 0 .9 3 6 0 2 0 . 0 0 .2 6 4 2 4 954 - 4 . 9 0 I 2 9 E - 0 4 1.51021 0 .9 2 4 7 9 0 .9 5 1 2 3 0 . 0 0 .2 6 4 2 4 955 - 4 . 5 4 7 8 3 E - 0 4 1.51021 0.9 2 7 4 3 0 .9 4 6 0 9 0 . 0 0 .2 6 4 2 4 956 - 4 . 30286E— 04 1.51021 0.9 4 5 7 0 0 . 93202 0 . 0
-6 .6 0 4 7 8 E -Q 3 EXTRAPOLATION WITH 15.3561 0 .2 6 4 2 4 957 - 1 . 4 1 0 3 3 6 - 0 4 I . C O 0 0 0 0.44378 0 .2 1 7 0 8 0 . 0 0 .2 6 4 2 4 958 -3 . 3 1 0 4 4 E - 0 4 1.51021 1.7 3 2 5 8 1 .3 3 7 9 3 0 . 0 0 .2 6 4 2 4 959 - 3 . 29673E—04 1.51021 0.99553 0*91928 0 . 0 0 .2 6 4 2 4 960 — 3 . 14772E-04 1.51021 0.9 5 4 4 9 0 .8 1 3 2 6 0 . 0 0 .2 6 4 2 4 961 -2 . 9 2 0 0 3 E - 0 4 1.51021 0 . 9 ^ 73 V 0 .8 1 0 8 ? 0 . 0 0 .2 6 4 2 4 962 - 2 . 7 6 8 6 4 E - 0 4 1.51021 0.9 4 7 8 8 0 . 78338 0 . 0 0 .2 6 4 2 4 965 -S.5737’5E-(5^ 1.51021 0.^2^S4 0 .8 7 2 3 8 0 . 0 0 .2 6 4 2 4 964 - 2 . 4 4 1 4 1 E - 0 4 1.5 1021 0. 94834 0 , 78 052 0 . 0 0 .2 6 4 2 4 965 - 2 . 29120E—04 1.51021 0 .9 3 8 2 5 0 .8 1 2 5 2 0 . 0 0 .2 6 4 2 4 966 - 2 . 1 4696E-04 1.51021 0.9 3 6 8 3 0 .7 6 9 2 5 0 . 0 0 .2 6 4 2 4 967 - 2 . 0 3 9 0 7 E - 0 4 1.51021 0 .94955 0 .9 5 0 02 0 . 0 0 .2 6 4 2 4 968 - 1 . 9 3 4 1 7 E -0 4 1.51021 0. 94836 0 .7 3 6 8 6 0 . 0 0.2 6 4 2 4 96 9 - 1. fi0364£-<54 1.5 1021 0 . 93233 0 .8 5 7 1 5 o . c 0 .2 6 4 2 4 970 -1 . 7 3 5 6 9 E - 0 4 1.51021 0 .9 6 2 1 5 0 .5 8 3 3 4 0 . 0 0 .2 6 4 2 4 971 - 1 . 6 4 6 8 8 E - 0 4 1.51021 0 .4 4 8 6 7 0 .2 6 5 7 2 0 . 0 0 .2 6 4 2 4 972 — 1 .5 3 8 9 9 E -0 4 1.51021 0 .9 3 4 3 4 0 . 0 0 . 0 0.2 6 4 2 4 97* ' - 1 . 4 5 3 7 6 E - 0 4 1.5 1021 0 .9 4 4 4 7 0 .9 4 4 4 7 0 . 0 0 .2 6 4 2 4 974 -1 .4 2 3 3 6 E - 0 4 1 .51021 0 .9 7 8 9 5 0 .9 7 895 0 . 0 0 .2 6 4 2 4 975 - 1 . 3 4 0 5 1 E - 0 4 1.5 1021 0.9415& 0 .9 4 1 6 6 O.o 0 .2 6 4 2 4 9 ' '76 - 1 . 2 8 4 4 8 E -0 4 1.51021 3.95808 0 .9 5 808 0.0 0 .2 6 4 2 4 977 - 1 . 2 1 5 3 4E-04 1.51021 0.94605 0.94605 0 .0 0 .2 6 4 2 4 978 - 1 . 1 7302E-04 1.51021 0.9 6 5 0 6 0 . 96506 0 . 0 0 .2 6 4 2 4 979 -l.l301v/E -04 1.51021 0.963*0 0 .9 6 3 3 0 0 .0 0 .2 6 4 2 4 980 - 1 . 0 7 4 0 8 E - 0 4 1.51021 0.95031 0 .9 5 0 3 1 0 .0 0 .2 6 4 2 4 981 - k . 0 4 6 b 6 E - 0 4 1.51 o i l 0 .97381 0.9 7 3 8 1 0 .0 0 .2 6 4 2 4 982 - 1 . 0 0 9 7 0 E - 0 4 1.51021 0 .9 6 5 1 4 0 .9 6 5 1 4 0 .0 0 .2 6 4 2 4 9^3 — 9 . j9 9 6 * E -0 5 1.5 1021 0.93084 o. 93064 0 .0 0.264249
fcND OF AD JO IN T CALCULATION - ITER A TIO N TIME 0 .1 2 6 M IN U ItS
COHVEftSEHCT l RH'ie m U N ' S r WrNIHm N ff'T H C SUH OF THE ggilW E r 'a r"TBg"ffn T PuES - RElATIvE A b so rp tion 0.9976392----- k " " o . 264U 68
GROSS NEUTRON BALANCE
GRP1
LFT LEAKAGE 2.6I320E IS
TOP LEAKAGE 2.44746E 15
RIT LEAKAGE 1*2803SE 16
BOT LEAKAGE -1 .28038E 16
FNT LEAKAGE 0 .0
BAK LEAKAGE 0 .0
B**2 LOSSES 0 .0
l/V LOSS 0 .0
XENON LOSS 0 .0
2 7.71249E 14 7.46484E 14 3.60568E 15 —3.6056CE 15 0 .0 0 .0 0 .0 0 .0 0.0
surf 3.3844!»I: 15 3.14345E 15 1.A4095E 16 —1.64095E 16 0 .0 0 .0 0 .0 0 .0 0 .0
GRP ABSORPTIONS OUT-SCATTER SOURCE IN-SCATTER TOTAL LGSSES TOTAL GAINS PROD/ABSGKP12
1.41979E 16 5.80160E 15
7.30318E 15 0 .0
2.65779E0 .0
16 0 .07.30318E 15
2.65618E 16 7.31932E 15
2.65779E7.30318E
1615
6.25798E-02 1.05741E 00
SUM 1.99995E 16 7.30319E IS 2.65779E 16 7.3031&E 15 3.38811E 16 3.38&11E 16
3 -D , 90 DEGREE ROTATIONAL SYHMETRY, QUARTER SECT1CN WITH BLACK ABSORBER9X9X3X2 GROUP, 486 POINTS STREAM OF C IT A T IO N CASES ORNL 72
PERTURBATION r e s u l t s ------- o e l t a - k / j k * d e l t a - S I WHERE S REPRESENTS MACRC. CROSS S EC TIO N S. LAMBDAIPHI* M PHI 1 = 3 .0 1 4 1 74E Cl
COMP NAME 1 CORE ZONE 1
GRP1
S IG A ,S lG R ,D B * * 2 0 .0
NU*SIGF 0 . 0
D I F F . CO£F. 0 . 0
B**20 .0
2 CORE ZONE 221
0 . 0-3 .3 1 3 3 0 6 E 01
O .C1 .2 5 3 7 9 6 E 02
0 . 0-1 .5 7 0 4 5 7 E - 0 1
J . O- 5 . 6 3 2 i l 9 E J l
3 AXIAL BLKT 121
- 3 . 3 2 l 2 0 « E O l -1 . 5 2 3 1 8 1 E 01
:>.4985l4fc5 .7 6 3 9 0 5 E
61Cl
-2 . 1 0 8 4 5 1 6 -0 1 -6 .9 S 4 2 7 6 E -0 2
— 3 . 752962E 01 -1 .8 2 7 8 1 7 E 01
2 -1 .4 4 4 1 3 9 E 01 2.2 2 4 1 0 7 E 01 —S .466733E—C2 — 1.256401E 01
T U H P ----------FTCRT;----------GRP~. " ' K r T fiSTFKP H AT I C EP S . KK"T O~5W P.' tO------------------- ----------------------------------------------------------------------------1 CORE ZONE 1 1 0 . 0 0 .0
2 OTO 0752 CORE ZONE 2 1 3.313306E 01 9.245243E 00
----------------------------------------------------- Z- l . T O S S i E ' f i n . m ' Z M F T J I ----------------------------------------------------------------------------------------------------------------------------------------------------------3 AXIAL 8LKT 1 1 1.523181F 01 5.877474E 00
---------------------------------------- g— 3; 7736?2E W "~ I.4T ^lSgE~Pl---------------------------------------------------------------------------------------------------------------------
END OF CASE - TOTAL CRu TIME HAS 0.33 MINUTES TOTAL CLOCK TIME WAS 1.49 MINUTES * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * ***************************************************************************************************************
* * * * * * * * * THIS JdB WAii RUN Ok) (>3-11-72 ON THE IBM 3 t>0/91 *********
3-D, 180 DEGREF ROTATIONAL SYMMETRY, HALF SECTION WITH BLACK ABSCRBER 9X18X3X2 GROUP, 972 POINTS STREAM OF CITATION CASES ORNL 72
3ENFP. AL CONTROL INPUT - SECTION 001
0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 1 0 4 0 0 01 0 0 0 1 0 0 0 1 0 0 . 1 1 0 1 0 0 0 0 0 0 0 0 0
100 100 10 2 3 0 0 1.500000E 00 9.999998E-03
6 o9.999999E
009
0 0 0 9.999999E
023
00 .0
0 0 0 12 6 12 1 .OOOOOOE 00
6 12 24
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 0 11 0 0 0 0 0 0 0 3 0 1 1 1 0 0 0 0 0 0 0 .9.999999E-05 9.999999E-05 9.999996E—02 0 .0
9 .999999E-05 2 . 500000E—01
9.9999S9E—05 9.500000E—01
9.999999E—05 5.000000E-01
0 .00 .0
LEFT,TOP,RIGHT,BOTTOM,FRONT,BACK BOUNDARY CONOITICNS ARE9.999996E-02 9.999996E-02 ROTATIONCl 801 9.999996E-02 OTO OTO”
ftOb RNO. CONSTANT FOR ALL- BftOU?'5' IN ZOTE— I — fS— 4T6'9*00<JE-0l------------------------------------------------------------------------------------------------------------1----------------------------------------
THRfe£ DIMENSIONAL SLAB GEOMETRY CX,Y,Z» WlOTH 3 .OOOOOOE 01 HEIGHT 6 .OOOOOOE 01 OEPTH 9.999999E-01ro----------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- -------------- H
- 4TfP'GIUN- S P E C IF IC A T IO N S
PTS REGION WIDTH3 9 .OOOOOOE 00 3 1.200000E 01 3 9 . COOOOOE 00
PTS3
REGION HEIGHT 9.000000E 00 3 1.200000E 01 3 9 . OOOOOOE 00 3 9 . OOOOOOE 00 3 1.200000E 01 3 9 .OOOOOOE 00
PTS REGION OEPTH3 1 .OOOOOOE 00
X—DIR. POINTS 5 Y-D IR . POINTS TS Z-O IR . POINTS 3
D IS T ANCES TO MESH' l N l f c m i lNrEKt-ACfc5---------------------------------------------------------------------------------
j n i s i . 2 3.000 3 6.000 4 9.000 5 13.000 6 17.000 7 21.000 8 24.000 9 27.000 10 30.000
I DIST.2 3.000
11 33.0P03
126. COO
36.0004
139.000
39.000b
141 3 .COO 4 3 .COO
615
17.00047.000
716
21.00051.000
817
24.00054.000
918
27.00U57.000
1019
30.00060.000
KB DIST? 0.333 3 0.667 4 1 . 0 0 0
D I S T A N U t S I U F L U X P O I N T S
J D IS f . 1 1.500 2 4.500 3 7.500 4 1 1 . 0 0 0 5 15.000 6 19.000 7 22.500 8 25.500 9 28.500
I D IS T •
X 1.500 t ‘t.buO 3 7.500 4 11.000 5 15.000 6 19.000 7 22.500 8 25.500 9 IU .50010 31.500 11 34.500 12 37.500 13 *1 .0 0 0 14 45.000 15 49.000 16 52.500 17 S5.500 18 58.500
KB DIST1 0.167 2 0 .500 3 0.833
ZONE tNPUt B Y T fff lf iN
PLANE NUMBER I1 2 3_____________________________2 2 33 2 I_____________________________3 3 12 2 21 2 3
ZONE HUMfi'Eft AT RCH"ME,'Sfc rWTERVAL
SPECIFICATION FOP LAVER NUMBER T
-------------j— 2 "3 •" ? - T ~ 8— I " B '
1 I 1 l 2 ? 2 3 3 32 1 1 l 2 2 2 3 3 33 1 1 l 2 2 2 3 a 34 2 2 2 2 2 2 3 3 35 2 ? 2 5 2 2 3 3 3 ‘6 2 2 2 2 2 2 3 3 37 3 3 3 2 2 2 1 1 18 3 3 3 2 2 2 1 1 19 3 3 3 2 2 2 1 1 1
10 3 3 3 3 3 3 1 1 111 3 % 3 3 3 3 1 1 112 3 3 3 3 3 3 1 1 113 2 2 2 2 2 2 2 2 214 2 2 2 2 2 2 2 2 215 2 2 2 2 2 2 2 2 216 1 1 I 2 2 2 3 317 ■ - 1 i i 2 2 2 3 3 318 1 l l 2 2 2 3 3
S P E C IF IC A T IO N FOR LAYER NUMBER 2
1 2 3 4 5 6 7 8 9
1 1 1 1 2 2 2 3 3 a2 1 1 1 2 ? 2 3 3 33 1 1 1 2 2 2 3 3 34 2 2 2 2 2 2 3 'i A5 ? 2 2 2 2 2 3- 3 36 2 2 2 2 2 2 3 3 57 3 3 3 2 2 2 1 l 18 ‘i i 3 2 2 2 1 1 T " ------------9 3 3 3 2 2 2 1 l I
“ 10“ ' 3 '4 a 3 J 3 1 1 i11 3 3 3 3 3 3 1 1 l12 3 3 3 3 3 3 1 1 l13 ? 2 2 2 ? 2 2 2 214 2 2 2 2 2 2 2 2 215 2 2 2 _ 2 2 .2 2 2 2
16 1 1 1 2 2 2 3 3 317 1 1 1 2 2 2 3 3 3I B 1 1 1 2 2 2 3 3 3
Sp e c if ic a t io n £or laye h number ?
1 2 3 4 5 6 / 0 9
1 1 1 1 2 2 2 3 3 32 1 I I 2 2 2 3 3 33 1 1 1 2 2 2 3 3 34 2 ? 2 2 2 2 3 3 35 2 2 2 2 2 2 3 3 36 2 2 2 2 2 2 3 3 37 3 3 3 2 2 2 1 18 3 3 3 2 2 2 1 1 19 3 S 5 2 2 2 1 1 1.
10 3 3 3 3 3 3 1 1 111 3 3 3 3 3 3 i 1 112 3 3 3 3 3 3 1 1 113 2 2 2 2 2 2 2 214 2 2 2 2 2 2 2 2 2
"1 5 2 2 2 2 2 2 2 ? 216 I 1 1 2 2 2 3 3 317 1 1 1 2 2 2 3 3 318 1 1 l 2 2 2 3 3 3
CORE STORAGE DIFFERENCE <WORDS) EQUAT i O N C C N S T A N T S t/n I N S T F A . ) OF STORED____ 1 70 1
EQUATION CONSTANTS HILL BE STORED IN CORE
NUMBER OF---- COLUMNS. ROWS. PLANES. CROuFS, UPSCAT, OOWNSCAT. REGIONS. ANO ZOMfcS__________9 16 3 2 0 1 18 3
MEMORY LOCATIONS RESERVED FOR DATA STORAGE----- 401)00MEMORY LOCATIONS USED FOR THIS PROBLEM------------- 9459 " ' 'MEMO0Y LOCATIONS NOT USED---------------- ------------------ 30501
219
9X18X3X2 GROUP. 972 POINTS STREAM OF CIIATJCN CAStS ORNL 72I V j? >=JL±«4Tigw “ HL.-BE DONE CM ROWS - 3 INNER 11ERATI0N(S1ITERATION FLUX CHANGE OC 1 A KU-2 MU..* K
1 -4 .4 1 8 3 7E-Q2 1.00000 -0 .08837 0.012S8 0 .0 0.3781672 -2.13820E-01 1.80966 4.6255 3 15.60164 - C .03707 0.3913813 -2.08785E-01 1.68319 0. 76 76 7 1.07 o45 1.11175 0.4015544 -1 .2 5 5 1 3E-01 1.60222 0.47565 0.73688 0.66446 0.4041925 -7# 7378 IE-02 1.55866 0. 53912 0.70 5C7 0.73541 0.4C44266 -6 .17429^-02 1.53 534 0.73619 0.61986 0.85351 0.4038747 -5.2S412E-02 1.52 314 0.8Q299 0.87579 0.90243 0 .402oOl8 -4.70117E-02 1.51684 0.8426 7 0.90119 0.92813 0.4013339 -4 .260S3E-02 1.51360 0.86366 0.91221 0.94107 0.399945
10 - 3 .90347E-02 1.51194 0.87716 0.91802 0.94827 0.39750011 -"3.60084E-02 1.51109 0.88646 0.92115 0.95252 0.39524312 T751666 6.89384 0.92285 0.95513 0.39281913 - 3 .10766E-02 1.51044 0.89970 0.92403 0.95694 0.39026314 -2.90186E-02 1.51033 0.90476 0.92621 0.95832
-3.23726E-01 EXTRAPOLATION WITH 10.8323 0.3561151$ -6 .763>2e-03 1.00000 0.22699 0.43794 11.03102 0.35483116 -1 .25302E-02 1.51024 1.83457 1.78535 O.C3913 0.35210317 1.2776 5T-35- 1.51023 1.00668 6.99132 1.16497 0.349010IB -1.23426E-02 1.5102? 0.95370 0.93182 0.98336 0.34605219 — 1•17975E—02 1.51021 0. 94403 0.92083 0.97416 0.34323320 -1.13108E-02 1.51021 0. 94744 0.92619 0.97398 G .34055321 -1.08649E-02 1.51021 0.94971 0.93056 0.97321 0.33/9d522 -1.04590E-02 1.51021 0. 95219 0.93356 0.97259 0.335 52423 -1.00951E-02 T . 51021 Cl. 95511 0.93675 0.97210 6.33316324 —9 .75609E-03 1.51021 0.95666 0.93935 0.97159 0.33089425 -9.43905E-03 1.51021 0.95806 0.94176 0.97118
-1.80691E-01 EXTRAPOLATION WITH 18.9639 0.28665526 -5 .629?8£-ff3 1.00000 0.59080 0.18272 19.12411 0.28643027 - 9 . 862V6E-03 1 51021 1.74206 1.74351 0.01794 0.28593526 -4 .54152E-63 1.51021 t). 9628$ 0.9^636 1.14535 0.28534429 -B.73238E-03 1.51021 0.90169 0.94183 0.96535 0.28475230 -7 .8 4 3 5 EE-03 1.51021 0.89037 0.92865 0.95799 0.28416731 -7.09373E-03 1.51021 0. 89 731 0.95405 0.95933 0.28358932 -6.44112E-03. 1.51021 0.90156 0.95030 0.96031 0.28302033 -5.87577E-03 1.51021 0.90635 0.95508 0.96113 0.28246034 -5.382?2E-Q3 1.51021 0.91070 0.95785 0.96185 0.28191235 -4 .95368E-03 1.51021 0.91534 0.95127 0.96233 0.28137*36 -4.58002E-03 1.51021 0.91999 0.97489 0.96300 0.26084837 -4 .24778E-03 1.51021 0.92321 0.93152 0.96346 0.280 33438 -3 .959126-03 1.51021 0.92808 0.99029 0.96372 0.27983239 -3 .6 9 8 1 IE-03 1.51021 0.9303 8 0.985S4 0.96446 0.27934340 -3.4V114E-63 1.51021 0.93515 0.98S97 0.96462 0.27886641 -3 .26580F-03 1.51021 0. 93 758 0.99243 0.96481 0.27840242 -3 .08222E-03 1.51021 0 .9407C 0.98186 0.96524 0.27795043 -2.91342E-03 1.51021 0. 94232 0.98 3 24 0 . 9o563 0.27751044 - 2 . 76566E-03 1.51021 0. 94652 0.97 836 0.96592 0.27708345 -2 .6 2 856E-03 1.51021 0.9478 0 0.97967 0.96600 0.27666746 -2 .50292F-03 1.51021 0.9497 0 " u . m w 0.96613 0 .2 7626347 -2 .38752E-03 1.51021 0.95151 0.97561 0.96618 0.27587248 -2 .28184E-03 i . 51021 0.95346 0.97 593 0.96612 Q .27549249 -2 .18844E-03 1.51021 0.95688 0.97219 0.96709 0.27512350 —2 .09510E—03 fT3 l021 0.95525 0.97025 0.9665V 0.27476551 -2.01076E-03 1.51021 0.95773 0.96490 0.96683 0.27441752 -1 .73W 2E -tf3 1 . SI 021 0.9^811 O .V fO il 0.96700 o .2 /4o b i53 -1.85889E-03 1.51021 0.96109 0.97282 0.96688 0.273754
55 -1 .72150E-P3 1.51021 0.96204 0.96587 0.967070.2734300.27 3 1 3 1
56 -1 .65957E-03 1.51021 0.96237 0.96975 0.96762 0.27283457 - 1 . 59663E-03 1.51021 0.96048 0.96341 0.96709 0.272546
ror oo
Sb -1 .5448 3E-03 1.51021 0.96601 0.96470 0.96768 0.27226759 -1 .49006E-03 1.51021 0.9630 5 0.96477 0.96734 0.27199760 -1 .43534E-03 1.51021 0. 96184 0.96639 0.96759
-3.86154E-C2 EXTRAPOLATION WITH 26.8688 0.26466361 -1 .65641E-04 1.00000 0.11524 0.12334 26.90595 0.26465462 -1 .99378E-04 1.51021 1.20347 1.23759 0.00303 0.26463163 - 1.94073E-04 1.51021 0.97320 0.85867 1.16629 0.2646046* -1 .76847F-04 1.51021 0.91106 0.78830 0.99011 0.26457865 -1 .6713 IE -04 1.51021 0. 94490 0.86573 0.98048 0.26455366 -1 .58489E-04 1.51021 0.94813 0.93109 0.98203 0.26452967 -1 .52171E-04 1.51021 0.95998 0 .88 893' 0.98303 0.26450668 -1 .46925E-04 1.51021 0. 96538 0.91671 0.97495 0.264484 .69 -1 .43290E-04 1.51021 0.97511 0.88640 0.97977 0.26446370 -1 .35601E-04 1.51021 0.9462 0 0.87183 0.98101 0.26444271 - 1 . 30534E-04 1.51021 0. 96251 0.85297 0.97687 0.26442372 -1 .24454E-04 1.51021 0.95330 0.93106 0.97812 0.26440473 -1 .2T653E-04 1.51021 0.9773 7 0.92595 0.97738 0.2643867* -1 .22547E-04 1.51021 1.00723 0.760G2 0.97922 0.26436975 -1 .1533 5E-04 1.51021 6.44103 0 .94 *34 0.97851 0.26435276 - 1 . 13130E-C4 1.51021 0.98077 1.00002 0.97770 0.26433777 -1 .07169E-04 1.51021 0.94721 0.50001 0.97963 0.26432178 -1 .07765E-04 1.51021 1.00545 1.11112 0.98130 0.264306 .79 -1 .02043E-04 1.51021 0.94680 0.80C01 0.97534 b . 26429280 -9 .9122 5E-05 1.51021 0.97123 0.62500 0.97678 0.26427881 - S . /142TJE=0'5" ' "1743735” 0.87905 0.40000 o . b i i ' t i 0.26426?82 -3 .15988E-05 1.43732 0.93631 l.OOCOC 0.94116 0.26425683 -fl".rS372E-65 1.43732 1.00284 0.50000 0.98014 0.264246
ENO Ut= EIGENVALUE CALCULAIION - ITERATION TIME 0.324 MINUTES
-OTWEgggWCE TNmCATION UV M to lM lllN li ffl'E SUH"OF TffE~SOuAHES UP"THE ft£ST P'u£j~ r£ la t1 v 5 —ABSORPTION 0.9966*76 ------k ~ o '.2 6*36'sl'
LfAKfiGE 1.31567E 16 TOTAL LOSSES 5.31567E 16 TOTAL PRODUCTIONS 1 .40464E 16 REACTOR POHER(UATTS) 2.63158E 05
ADJOINT PftOBTCfi FOLLOWS ITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3 K
1 4 .60767E 28 l.O O O O O ********** -0 .01468 0 .0 0.2642462 1.39662E 02 1.80966 139.66173 4.59437 0 .0 0.2642463 5.01199E 01 1.68019 50. 47873 0.93729 0 .0 0.2642464 9.34012E CO 1.60222 9.52648 0.6BB09 0 .0 0.264246
' 5 2.55742E 00 1.55866 2.83123 0.71442 0 .0 0.2642466 1.23378E 00 1.53534 1.71621 0.83505 0 .0 0.2642467 7.59090E-P1 1.52314 1.57254 0.88?14 0 .0 0 .2642468 5 . 32166E-01 1.51684 1.23415 0.91872 0 .0 0.2642469 4.04388F-01 1.51360 1. 16428 0.93353 0 .0 0.264246
10 3.23014E-01 1.51194 1.12179 0.94167 0 .0 0.26424611 2.66808E-01 1.51109 1.09260 0.94758 0 .0 0.26424612 2 . 25665E-01 1.51066 1.07146 0.94908 0 .0 0.264246
' 13 " 1.94406E-01 1.51044 1. Ot>588 0.95083 0 .0 0.26424614 1.70071E-01 1.51033 1.04489 0.95302 0 .0 0 .26424615 1.3B344E-01 1.51027 T.OT435 0.9531? 0 .0 0.26424616 1.3403 5E-01 1.51024 1.02556 0.95337 0 .0 0.264246
.... 17 1 .2n339E-01 1.51023 1.01 til 6 0.95368 0 .0 0.26424618 1.08709E-01 1.51022 1.01206 0.95373 0 .0 0.26424619 "" S.57124E-62 T . 51 <521 1.00676 0.95421 0 .0 0.264246?e 9.00373E-02 1.51021 1.00215 0.95460 0 .0 0.26424621 8 .24490E-02 1.51021 0. 99817 0.95517 0 .0 0.26424622 7.57627E-02 1.51021- 0.99467 0.95576 0 .0 0.26424623 6.98347E-02 1.51021 0.49159 0.95611 0 .0 0.26424624 6 .45485E-02 1.51021 0.98885 0.95677 0 .0 0.26424625 5.3805BE-62 1. 51021 — 0 .9 3 5 3 5 " 0.95740 0 .0
1.95005E 00 EXTRAPOLATION WITH 34.5558 0.26424626 - 6 . l98§9E-03 1.00000 -0 .10984 -0 .45745 0 .0 0.264246 '27 -1 .13513E-02 1.51021 1.81993 1.73171 0 .0 0.264246
’ ?8 -1 .14754E-02 1.51021 0.99946 1.C1389 0 .0 0.264246 129 -1 .09924F-02 1.51021 0. 94691 0.96210 0 .0 0.264246
221
30 -1.03753E-02 1.51021 0.93349 0.94685 0 .0 0.26424631 - 9 . 79960E-03 1.51021 0.93471 0.94946 0 .0 0.26424632 -9 .26727E-U * 1.51021 0.93641 0.95050 0 .0
-1.56Q72E-01 . EXTRAPOLATION WITH 16.6857 0.26424633 -5.56350E-03 l.OOOOU ~ 0.59477 0.29380 0 .0 S .26424634 ■ 1. 3r* A”3t£— 02 1.51021 1.79549 1.68216 0 .0 0.264246
'35 -1.00180E-02 1.51021 0.98728 0.95659 0 .0 0.26424636 - g . ^ s ^ E - o a 1.51021 0.9433 7 0.88955 0 .0 0.26424637 -8.97044E-02 1. *>1021 0.93070 0.87756 u .o 0.26424633 -8.42512E-03 1.51021 0.93078 0.87404 0 .0 0.26424639 -7.90620E-03 1.51021 0.93050 0.86965 0..0 0.26424640 -7 .4188 !E -03 1.51021 0.93093 0.87C26 0 .0 0.26424641 -6 .95586E-03 1.51021 0.93064 0.86 964 0 .0 0.2642464? -6.52289E-03 1.51021 0.93123 3.87416 0 .0 0.26424643 -6 . 12116E-03 1.51021 0.93229 0.93581 0 .0 0.26424644 -5 .73826E-03 1.51021 0.93171 0.93308 0 .0 0.26424645 -5 .386116-03 1.51021 0.93325 0.93516 0 .0
-7.68814E-02 EXTRAPOLATION WITH 14.1980 0.26424646 -4 .89354E-04 I . 00000 0.09037 0.33146 0 .0 0.26424647 - 8 . 51691E-04 1.51021 1.73959 1.80772 0 .0 0.26424648 -8 .26538E-04 1.51021 0. 96964 0.99148 0 .0 0.26424649 -7 .71821E-04 1.51021 0.93303 0.95488 0 .0 0.26424650 - 7 . 10189E-04 1.51021 0.91944 0.94 502 0 .0 0.26424651 -6 .54757E-04 1.51021 0.92129 0.93971 0 .0 0.264246~ W -6 .63497E-04 1.51 O il 6.9 2 111 "Ty.4551(i 6 .0 0.26424653 -5 .58972E-04 1.51021 0. 92566 0.93042 0 .0 0.26424654 -5 .1623 6E-04 1.51021 0.92303 0.94697 0.0 0.26424655 -4 .8 6 9 1 OE-04 1.51021 0.94271 0.95420 0 .0 0.26424656 -4 .52399E-04 1.51021 0. 92 867 0.93850 0 .0 0.26424657 - 4 . 20153E-04 1.51021 0.92830 0.94014 0 .0 0.26424658 -3.42199E-04 1.&1051 0.93307 6.924C7 0.6 0.26424659 -3 .62277E-04 1.51021 0.92335 .95407 0 .0 0.26424660 -3.43382E-04 1.51021 0.94750 U .94490 0 .0 0.26424661 -3.16799E-04 1.51021 0.92227 0.93065 0 .0 0.26424662 -2.99811E-04 1.51021 0.94608 0.95299 0 .0 0.2642466? - 2 . 79784E-04 1.51021 0.93292 0.929S7 0 .0 0.26424664 -2.63870E-04 1.51021 0.94286 0.92909 0 .0 - 0.26424665 -2 .49386E-04 1.51021 0. 9448C 0.95234 0 .0 0.26424666 -2 .3573 6E-04 1.51021 0. 94503 0.95495 0 .0 0.26424667 -2.21670E-04 1.51021 0.94011 0.95280 0 .0 0.26424668 -2 .14279E-04 1.51021 0. 96644 0.91176 0 .0 0.26424669 - 2 . 10345E-.04 1.51021 0.98143 0.94560 0 .0 0.26424670 -2 .694516-04 1.51021 6.94554 0.93604 0 .0 0.26424671 -2 .0343 IE -04 1.51021 0.97105 0.965 89 0 .0 0.26424672 -2 .00808E-04 1.51021 0.98691 0.91502 0 .0 0.26424673 -1 .94848E-04 1.51021 0.97012 0.93810 0 .0 0.26424674 -1 .92702E-04 1.51021 0.98879 0.94226 0 .0 0.26424675 - 1 . 87755E-04 1.51021 0.97414 0.92S93 0 .0 0.26424676 -1 .63582E-04 1 .6 io 2 i 6.47754 IT . 41514 O.o 0.26424677 -1 .80244E-04 1.51021 0.98164 0.95885 0 .0 0.26424678 - 1 . 76489E-04 1.51021 0. 97899 0.88180 0.0 0.26424679 - 1 . 71006E-04 1.51021 0. 96876 0. 9878B 0 .0 0.26424680 -1 .67668E-04 1.51021 0.98031 0.93834 0 .0 0.26424681 -1 .6 3 6 1 5E-04 1.51021 0.97566 0.86848 0 .0 0.26424662 -1 .54631E-64 'T . T t a r r ' 6.'47590 0.45461 O.o 0.26424683 -1 .54316E-04 1.51021 0.96625 0.92069 0 .0 0.26424684 -1 .50800E-04 1.51021 0.97706 3.93164 6 .6 0.26424685 -1 .47223E-04 1.51021 0.97614 0.925S7 0.0 0.26424686 -1 .43468^-04 1 .5 10 2 1 0.97435 0.62004 6 .0 0.26424687 - 1 . 39296E-04 1.51021 0.97078 0.87808 0 .0 0.264246BB -1 .341 /Of: -TT4 i • I 0.y6'30/ ' l.OUUUJ CT.0 U.76424689 -1 .34408E-04 1.51021 1.00164 0.91670 0.0 0.26424690 - 1 . 2552 7E-04 1.51021 0.93380 0.87882 0 .0 0.26424691 -1 .25885E-04 1.51021 1.0027 2 0.93106 0 .0 0.26424692 - 1 . 0895 7E-04 1.43732 0.86542 0.74076 0 .0 0.26424693 - 9 . 8526 5F-05 1.43 732 0.90417 0.65001 0 .0 0.264246
r croro
94 - 9 . 57847E-05 1.43732 0.97208 1.00001 i0 .0 0 .264246
END OF ADJOINT CALCULATION - ITERATION TIME 0.261 MINUTES
CONVERGENCE INDICATION BY MINIMIZING THE SUM pe THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 0.99'63478 K 0.2640337
- '
GROSS NEUTRON BALANCE
GRP1
LFT LEAKAGE 5 .06085E 15
TOP LEAKAGE 2.44749E 15
R iT LEAKAGE 0 .0
BOT LEAKAGE 2.61304E I S
FNT LEAKAGE 0 .0
BAK LEAKAGE 0 .0
8**20 . 0
LOSSES l/V LOSS 0 .0
XENON LOSS 0 . 0
2 1.51769E 15 7.46460E 14 0 .0 7.71187E 14 0 .0 0 .0 0 .0 0 .0 0 .0
SUM 6.57854E 15 3.19395E 15 0 .0 3.3842 2E 15 0 .0 0 .0 0 .0 0 .0 0 .0
grp ABSORPTIONS OUT-SCATTER SOURCE IN-SCATTER TOTAL LOSSES TOTAL GAINS PROD/ABSGRP12
2.83966E 16 1.16033E 16
1.46069E 16 0 .0
5. 31566E 16 0 .0
0.01.46069E 16
5.31249E 16 1.46386E 16
5.31566E 16 1.46069E 16
6.25801E—02 1.05740E 00
SUM 3.99999E 16 1.46069E .16 5. 31566E 16 1.46069E 16 6.77635E 16 6.77635E 16
AVERAGE FLUXES BV ZONE AND GROUP
ZONE 1— CORE ZONE 1575 575
T0NE 2— CORE ZONE 21.89858E 15 5.24331E 1*
ZONE 3— AXIAL BLKT 1- 1— 1.48318E 15 "5.70637E 14
ZONE AVERAGE POWER DENS IT IES(WATTS/CCI 0 .0 1.40576E 02 0 .0
THE MAXIMUM POWER DENSITY(WATTS/CO AT ROW 7 ANC COLUMN 4 ANO LINE 1 IS 1.847873E C2
THE AVERAGE POWER DENSITY ALONG ROW 7 IS 1.551559E 02 AND THE RELATIVE PUHEK DENSITIES!FRACTION OF AV.ERAGEI ARE 0T0 575 0 .6 1.190978^ 00 1.070266E 00 7.387553E-01 0 .0 0 .0 ' 0 .0
THE AVERAGE POWFR DENSITY DOWN COLUMN! 5 T5 1.375760E 02 ANC THE RELATIVE POWER DENSITIES ARE4.554379E-01 5.720136E-01 7.236242E-01 1.0101296 00 1.240734E 00 1.338956E 00 1.343164E 00 1.320690E 00 1.29S71BE 00OTO H570 575 1.300817^ 00 1.220501E 00 1.009924E 00 7.356673E-01 5.879741E-01 4.709763E-01
T HE A V EN G E POWm DENSI TY ALC1MG CIN E -1— 1~!> l . a 4 / g g 7 E~a7 " 'AND I HE RELAT IVE POdEft b E K S I T IE S Ar E------------------------------------------------------------------1.00001 IE 00 1.000001E 00 9.999876E-01________ _______________________________;____________________________________________________________________________
223
3-D, 160 DEGREE ROlAT IONAL SYMMETRY, HALF SECTION WITH BLACK ABSORBER 9X18X3X2 GROUP, 972 POINTS STREAM OF CITATION CASES ORNL 72
CUMULATIVE HEAT GENERATION RATE(Mwf/CM**2I - FLCW FRCM bOTTCH TO TOP
PLANE NUMHER I- - - _ _ _ _ _ _
1 2.325E 03 2.B31E 03 3.321E 03 6.922E 03 7.748E 03 7.459E 03 1.861E 03 1.756E 03 1.691E2 2.32SE 03 2.831E 03 3.321E 03 6.710E 03 7 .4 U E 03 7.059E 03 1.861E 03 1 .7 5 6 E 0 3 1.691E3 2.325E 03 2.831E 03 3.3~-lS 03 . 6.443E 03 7.010E 03 6.593E 03 -1.861E 03 1.756E 03 1.651E4 2.195E 03 2.670E 03 3.119E 03 6.016E 03 6.457E 03 5.988E 03 1.861E 03 1.756E 03 1.6S1E5 1.855E 03 2.253E 03 2.619E 03 5.396E 03 5.758E 03 S.278E 03 1.8616 03 1.756E 03 1.6S1E
~~b 1.392E 03 1.693E 03 1.9796 03 4.6876 03 5.038E 03 4.625E 03 1.861E 03 1.756E 03 1.691E7 1.139E 03 1.390E 03 1.636E 03 4.041E 03 4.432E 03 4.152E 03 1.B61E 03 1.756E 03 1.6S1E8 1.139E 03 1.390E 03 1.636E 03 3.491E 03 3.947E 03 3.830E 03 1.861E 03 1.756E 03 1.6S1E9 1.139F 03 1.39CE 03 1.636E 03 2.951E 03 3.^84E 03 3.540E 03 1.861E 03 1.756E 03 1.691E
"TO 1.139E 03 1.390E 03 1.636E 03 2.6846 03 3.257E 03 3.401E 03 1.861E 03 1.756E 03 I.691E11 1.139E 03 1.390E 03 1.636E 03 2.684E 03 3.257E 03 3.401E 03 1.861E 03 1.756E 03 1.691E
"T? 1.1^96 03 r i W B T T r ■ X.636E 03 2.6846 63 3.25tE 03 3.4016 03 1.861E 03 1.756E 03 1.691E13 8.968E 02 1.099E 03 1.306E 03 2.326E 03 2.905E 03 3.100E 03 1.632E 03 1.55SE 03 1.505E14 4.526E 02 5.610E 02 6.872F 02 1.632E 03 2.190E 03 2.442E 03 1.071E 03 I.Q41E 03 1.016E15 1.253E 02 1.574E 02 1.9916 02 1.C19E 03 1.485E 03 1.717E 03 3.69SE 02 3.633E 02 3.564E13 070 OTO 070 5.889E 02 9.2106 02 1.092E 03 OTO oT5 o7o“17 0 .0 0 .0 0 .0 3.157E 02 5.066E 02 6.073E 02 0 .0 0 .0 0 .0TS------ 575--------------- 573--------------- 575--------------- 57 7W 5T— 1 .576E 02 i .& $ ? 6 02 0 .6 ---------------oTo---------------oTo-
PLANE NUMBER 2
-------------- 1----------------- 2----------------- 3----------------- 5----------------- 5----------------- S----------------- 7----------------- S----------------- 91 2.325E 03 2.831E 03 3.321F 03 6.922E 03 7.748E 03 7.4S9E 03 1.861E 03 1.756E 03 1.691E
~1-------2.325E 03 2 . (55IE 03' 3.32IE OS 6 .7 10 r0 3 — 773111 03 /.0S46 o3 1.S&1E 03 "i.7 5 6 E ~0 3 l '.o s iE3 2.325E 03 2.B31E 03 3.321E 03 6.443E 03 7.010E 03 6.593E 03 1.861E 03 1.756E 03 1.691E
~4 2.195E 03 2.670E 03 3.118E 03 6 . 016E 03 6.457E 03 5.988E 03 1.861E 03 1.756E 03 1.6S1E5 1.855F 03 2.252E 03 2.619E 03 5 .396E 03 5.758E 03 5.278E 03 1.661E 03 1.756E 03 1 .69 IE
~6 1.392E 03 1.693E 03 1.979E 03 4.687E 03 5.038E 03 4.625E 03 1.861E 03 1.756E 03 1.691E7 1.139E 03 1.390E 03 1.636E 03 4.041E 03 4.432E 03 4.152E 03 1.861E 03 1.756E 03 1.691E
~5 1.139E 03 1.390E 03 1.636E 03 3.491E 03 3.$47E 03 3.8306 03 1.861E 03 1.756E 03 1.691E9 1.139E 03 1 .39OE 03 1.636E 03 2.951E 03 3.484E 03 3.540E 03 1.861E 03 1.756E 03 1.6S1E
TO 1.139E 03 1.390E 03 1.636E 03 2 .684d OS 3.257E 03 3.401E 03 1.861E 03 1 .7 5 6 E 0 3 1.6S1E11 1.139E 03 1.390E 03 1.636E 03 2.684E 03 3.257E 03 3.401E 03 l.B b lE 03 1.75&E 03 1.6S1E12 1.139E 03 1.3906 03 1.636E 03 2.6846 03 3.257E 03 3.401E 03 1 .8b lE 03 1 .7 5 6 E 0 3 1.691E13 8.968E 02 1.099E 03 1.306E 03 2.326E 03 2.905E 03 3.100E 03 1.632E 03 1.555E 03 1.5G5ET ? 4.526E 02 5.610E 02 6.U72E 02 1.6326 03 2.190E 03 2.4426 63 1.071E 03 1.0416 03 1.016E15__ 1.253E 02 1.574E 02 1.991E 02 1.019E 03 1.485E 03 1.717E 03___3.695E 02 3.633E 02 3.564E
1 5 OTO 075 STO 5.8896 02 9.2106 02 1.092E 03 oTo OTO 070~17 0 .0 0 .0 0 .0 3 . 157E 02 5.066E 02 6.073E 02 0 .0 0 .0 0 .0
I B 57c 5715 9 .7196 01 1.576E 02 1.8976 02 oTo 57o oTo”
PLANE .NUMHfcR— T ---------------------------------------------------------------------- ---------- -----------------------------------------------------------------------------------------------------------------------------
------------------------------------ 2------------------------- 5------------------------- 5------------------------- s------------------------- 5------------------------- t ------------------------- g------------------------- 9
1 2 .3 2 5 E 03 2 .8 3 1 E 03 3 .3 2 1 E 03 6 .9 2 2 E 03 7 .7 4 7 E 03 7 .4 5 9 E 03 1 .8 6 1 E 03 1 .7 5 5 E 03 1 .6 9 1 E1 2 .3 2 5 E 03 2 . 8 3 IE 03 3 .3 2 1 E 03 6 . 7 lO E “'03 7 .411E 03 7 .0 i )9 E 03 1 .8 6 1 E 03 1 .7 5 5 E 03 1 .6 9 1 E3 2 .3 2 5 E 03 2 .8 3 1 E 03 3 .3 2 1 E 03 6 .4 4 3 E 03 7 .0 1 0 E 03 6 .5 9 3 E 03 1 .861E 03 1 .7 5 5 E 03 1 .6 9 1 E
■5---------2 . B S E A3 2 ;~&7 0h 03— 3 . n a g~73 6; ' gl 6b~ q3— U3 5 .9 0 S E 03— n B 6 IF D 3 " 1 . 755E 03— l ' .6 4 1 E5 1.B5SE 03 2.252E 03 2.619E 03 5.396E 03 5.758E 03 5.278E 03 1.861E 03 1.755E 03 1.691E6 1.392F 03 1.6936 03 1.979E 03 4 . 686E 03 5.0386 03 4.6256 U3 1.861E 03 1.755E 03 1.651E7 1.139E 03 1.390E 03 1.636E 03 4.041E 03 4.432E 03 4.152E 03 1.861E 03 1.755E 03 1.691E8 1.139E 03 1.390E 03 1.636F 03 3.491E 03 3r947E 03 3.330E 03 1.861E 03 1.755E 03 1.691E9 1.139E 03 1.390E 03 1.636E 03 2.951E 03 3.484E 03 3.540E 03 1.861E 03 1.755E 03 1.691E
030303030303030303030303030302
030303030303030303030303
_030302
030303"530303030303
l o ' l . l i 9 E 03 1.390EI . I O A F
0303
1.636E 1 .636E
0303
2.684E2.684E
0303
3.257E3.257E
0303
3.4C1E3.401E
0303
1.861E1.861E
0303
1.755E 1. 755E
0303
1.691E 1.691E \ .AQ16
030303l l
1 il a l i Y C1.139E 03 1.390E
1 flQQE0303
1.636E1.306E
0303
2.684E 03 2.326E 03
3.257E2.905E
0303
3.401E3.100E
O i03
1.B61E1.632E
0303
I*1.555E 03 1.505E 03
03131415
Q«9oofc4.52661.253E
020?
5.610E1.573E
0202
6.872E1.991E
0202
1.632E1.019E5 .889E
03030?
2.190E 1.485E 9 .2 10E
030302
2.4<V2E1.717E1.092E
030303
1.071E3.695E0 .0
0302
1.041E3.t»33£0 .0
QZ 3. 56<VE0.0
02
16 0 .0 0# 00 .0 3.157E 02 5.066E 02 6.073E 02 0 .0 0 .0 0*0 .
171R
0*00*0 0 .0 0 .0 9.719E 01 1.576E 02 1.897E 02 0 .0 U* 0
rorovn
3 -0 , IBP DEGREE ROTATIONAL SYMMETRY, HALF SECTICN WITH BLACK ABSCBBER9X18X3X2 GROUP, 972 POINTS STREAM OF CITATION CASES ORNL 72
»SftruA8/»riON ftESULTS— OELTA-K/(K*DELTA-S) WHERE S REPRESENTS MACRC. CROSS SECTIONS. LAMB0A(PHI* M P H I> = 6.027269E 0)
COMP NAME GRP 1 CORE ZONE 1 1
SIGA,SIGR,0B**2 0 .0
NU*SIGF 0 .0
OIFF. COEF. 0 .0
B**20.0
22 CORE ZONE 2 1
0 .0—3.313319E 01
0 .01.253829E 02
0 .0-1.570249E-01
0 .0-5.632642E 01
23 AXIAL BLKT 1 1
- 3 . 322639E 01 -1.523828E 01
3.498450E 5 .766483E
0101
-2.109395E—01 -6.982625E-02
-3.754579E 01 -1.B28592E 01
2 -1.445229E 01 2.225041E 01 -B.472949E-02 —1.257349E 01
tbrp--------rare— ’ sep . x - — siBsiPnowAU- GftPs; w ro sap.' ki-------------------------------------------------------------------------------------------------------------1 CORE ZONE 1 1 0 .0 ______________ OjO_________________________________________________________________________________________________________________
2 0 .0 0 .02 CORE ZONE 2 I 3.313319E 01 9.244864E 00___________________ ;________________________________________________________________________________
2 I.I94100E 02 3.322639E 013 AXIAL BLKT 1 1 1.523828E 01 5.879807E 00
------------------------------------ r T T i m m o i 61-------------------------------------------------------------------------------------------------------------------------------
END OF CASE - TOTAL CPU TINE WAS 0.63 MINUTES TOTAL CLOCK TIME WAS 2.40 MINUTES^^^^^^t****************«********************** ********** ***************************************************____________***************************************************************************************************************
* * * * * * * * * Yh I s JOB WAS kUN ON 03-11-72 ON THE IBM 3 6 0 / 9 1 * * * * * * * * *
roroo\
F I C T I C I O U S P L U TOMIUA1 EXPOSUPF GIVEN A F I X E D SOURCE1X2 GROUP, 2 POINTS STREAM OF CITATION CASES ORNL 72
MICROSCOPIC CROSS-SFCT ION UPDATING FOLLOWS
♦♦♦♦♦♦♦CONTROL OPTION IS
NEW CROSS SECTION TAPE 8 MADE
MICROSCOPIC CROSS-SECTION UPDATING FOLLOWS
♦♦♦♦♦♦♦CONTROL OPTION IS
CKO'S 5 S EC T I ON' SET ADOE'tT ra ~ T APfc"5'
MICROSCOPIC CROSS-SECTION UPDATING FOLLOWS
GENERAL CONTROL INPUT - SECTION 001
I 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 01 1 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
too lo o T5 5 3 0 5 5 0 0 5 5 0 0 0 0 0 0 12 6 12 6 12 241.500000E 00 5.000000E-01 9.999999E 09 9.999999E 23 0»0_______________ 1.0000006 00________________
OEPLFTI ON HISTORY INPUT - SECTION 002
2 4 2 0 1 0 0 0 - 5 0 0 1 0 0 0 0 0 0 0 0 0 1 0 05.9000C0E 03 2 .OOOOOOE 01
9.999998E- 5 . OOOOOOE
-0301
C.O5 .OOOOOOE 01
l.OOOCCOE3.00000QE
0001
9.999993E—31 3 . OOOOOOE 01
l.OOOOOOE 3 .OOOOOOE
0001
1 1 O O O C I O O I O O O O O O O O O O O O O O 1 0 0 0 3 1 2 0 0
NEUTRON FLUX PROBLEM DESCRIPTION - SECTION 003
0 0 0 0 1 0 0 0 0 0 1 1 1 1 0 0 0 C 0 1 0 0 0 09.999999E-05 I.OOOOUOc-65 9 .9 9 9 9 5 ^ -0 5 9.999999E-05 9.9999996-0^ 5V00.0________________0 .0 l.OOOOOOE 00 9.5000C0E-Q1 l.OUOQOOE 00 0 .0
LEFT,TOP,RIGHT,BOTTOM,FRONT,HACK BOUNDARY CONDITIONS AREo lo (5T5 575 "if.<5 4.692000E-01 4.6920006-01
’ ONE O I^N SIOTm rSLABTiEO flm Y m — BTBTH— l.flBWWtrF ft ft-----------------------------------------------
227
REGION SPECIFICATIONS PTS RFC,ION WIDTH
1 l.OOOOOOE OO
X-OIR. POINTS 1
DISTANCES TO MESH INTERVAL INTERFACES
J ~ D IST.7____1 .000
DISTANCES TO FLUX POINTS
J DIST. 1 0.500
ZONE INPUT BY REGION 1 ____
ZONE NUMBER AT FACH MESH INTERVAL
1
1 1
DESCRIPTION (IF REACTOR ZONES
7N TO ZN SUB-ZNS SIGMA-SET ID CLASS DPL NEX NAME1 1 0 1 0 0 0 0 EVERYBOOIES
DESCRIPTION OF MICROSCOPIC CROSS SECTIONS
STf FJDTS 5iTF5 uF5C fTBSC , t it l e1________ 6 2________ 0________ 1___________ UNREAL PLUTCNIUH DATA SET 1
GROUP UPPER ENERGY MFAN ENERGY 1/V X-SECTION DIST.FUNCT1 1 .000COPE 07 l.OOOOOOE 05 2.300000E-09 1.000000_____________2 6.000000E—01 2.000000E-01 X.599999E-06 0 .0
SUM 1.000000
INPUT NUCLIOE OENSlTIES(NUCLIDE NUMBER - DENSITY)
ZONES 1- I SUB-ZONE INDICATOR 0 AND CONTROL CPTION 05 6 .<JoonoE-0 2 T5 i.ot<Jc^e-d3 B 1 . 06000^-02
FIXED SOURCF INPUT SECTIUN 026
20N?-S0URfF<N/CC-$EC)I 2 •50000E 14
SOURCE DISTRIBUTION AND SUM7 . n o < ' f ' t - n 3 . 0 0 0 0 E - 111 1 . 0 0 0 0 0 0 0
TfrtAL 1Xfc[> SOURCE 2. 500000E 14 N/iEC
DECAY CONSTANTS INPUT FfirH CARDS
r S1GMA-SETS F I
228
NUC DFCAY CN ST.17 I . 71000E—09________________________________________________________________________________________________________________________ 0 0 ,0________ 0 0 .0 ____0 0 .0____O 0 .0_0 0 .0
CARD INPUT OF YIELD DATA_________________________________________________________________________________________________________________
SIGMA-SCTS 1 - I
F IS S . NUCS_________________________________________________________________________________________________14 15 16 17 0 C 0 0 0 0 0 0 0 0 0 0 C 0 0 0
YIELO FRACTIONS TO NUCLIOE 911.000000? 00 l.OOOOOOE 00 l.OOOOOOE 00 1 .OOOOCOE 00
NUCLIDE CHAIN DESCRIPTIONS
SIG.SET 1 THROUGH 1 CONTAIN 2 CHAINS
DECAY CAPTURE / YIELD NUCLIDE 14 15 16 17
NEW CHAIN STARTS14 0 .0 0 .0 i? O 0 .015 0 .0 C.O 0 .0 c . o16 0 ,0 0 .0 0 .0 0 .017 6 .0 0 .0 0 .0 0 .0
NEW CHAIN STARTS91 1.000000 0 1.0000000 1.0000000 1.0000000
CHAIN ARRAY j____ 1» 2 2 3 4 5 0 6 0 0
FISSILE NUCLIDES---- 14 16FERTILE NUCLIDES----- 15______________________________________________________________________________INTERMEDIATE N UCLI UFS-------NONE S P E C I F I E DOTHER NUCLIDES---- 17STRUCTURAL NUCLIDES-----NCNE SPECIFIEDSPECIAL NUCLIDES---- 5F TSSIDN PRODUCT NUCLIDES-------NINF SPECI FI ED
fORF stop^ge—dTfferfnce TworijsI eoIFaTTo^ ^ unstaTJTs !7 o TnsT ead- of- STORED 4
EQUATION CONSTANTS WILL BE STORED IN CORE
NUMBER OF---- COLUMNS, f<OWS, PLANES, GROUPS, UPSCAT, OOWNSCAT, REGIONS, AND ZONES 1 1 1 2 0 1 1 1
M^mOryMEMORY
LflCATldtofe hESERVED FliR DAtA STokAfif— ’ 466dd LOCATIONS USED FOR THIS PROBLEM------------ 3537
MEMORY LOCATIONS NOT USED----------------------------------- 36063
Fit/\itioos p u n o m u w exposure g iv e n a f ix e d source1X2 GROUP, 2 POINTS STREAM OF C I T A T I O N CASES ORNL 72
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOK C Y C L E I CYCLE TIME 0 . 0 DAYS TOTAL TIME 0 . 0 DAYS
A F I X ED SOURCE PROBLEM L INF RELAXATION MILL BE
FOLLOWSDONE ON ROWS - 1 INNER H E R A T 1 0 N ( S )
I T ER AT I ON1
FLUX CHANGF 8.85013E 01
BETA1 .0 00 00
MU-1 1 77 .0 02 50
M U - 2 0 .0
MU-30 . 0
DRIVE FACTOR 7 . 1 4 4 2 1 0 - 0 1
BALANCE1. 399734
23
- 2 . 8 4 5 6 2 E - 0 1- 3 . 8 5 1 3 2 E - 0 2
1 .0 0 0 0 0 1 .00000
- 0 . 2 8 7 7 80. 09 6 83
- 0 . 2 8 7 7 8 - 0 . 1 1 1 8 3 0 . C 4 U 0 0 . 1 4 8 17
7 . 1 7 71 0 D- 0 17 . 1 8 6 8 5 0 - 0 1
0 .9 9 54 1 80 .9 9 86 4 4
45
- 5 . 4 8 8 4 0 E - 0 3 - 5 . 4 93 76 E- 04
1 .0 00 001. 00300
0. 13702 0. 09955
0 . 3 0 1 6 10 . 2 3 9 5 7
0 .1 1 89 20.06042
7 . 1 8 9 1 6 0 - 0 1 7 . 18944D-01
0. 99 9 67 B0.999961
6 3 . 8 I 4 ? 0 F - O 5 1.00000 - 0 . 0 6 9 4 0 - 6 . 0 6 4 7 7 - 0 .0 9 42 6 7 . 18942D-01 1. 000003
END OF FIXED SOURCE CALCULATION - I T ER AT I ON TIME CTo MINUTES
LEAKAGE 0 . 0 TOTAL LOSSES 3 .3 8 V 2 6 E 14 T OT AL PRODUCTIONS 8 .8 92 61 E 13 REACTOR POWER(WATTS) 1 .08243E 03
FICTICIPUS PLUTQMIUM EXPOSURE GIVEN A FIXED SOURCE__________________________1X2 GROUP, 2 POINTS STREA* OF C IT AT ION CASES ORNL 72
GROUP 1 FLUX
11 1.334D 14
GROUP 2 FLUX
________ 1I 2.371D 13
NUCLlDE R fA t T t O N RAtES NORMALIZED fo 3 .3 8 9 2 5 S t 14 TOTAL L CSSCS ‘THE AHOUNTIKGI I S AT DEPLETION T I HE 0 . 0 ______________ OAVS> AND THE REACT IOM RATES ARE AT OEPLLT LON TIME 0 . 0 _____________ DAYS
TOTAL NuCL! Dr REiCTION RATES
NUC. A“ Q‘JNTtKG» ABSURPT1UNS CAP(URES PROL'UCI IONSGRAPHITE 5 1 .1 95 51b-03 1 .6 7915F-06 1 ' ( .M IS E -G b 0 .0PU-239 14 3.96843E-04 1.171S1E-01 4.07070E-Q2 2.09508E-01PU-240 lb 3.98503E-03 <J.ol070E-0l 8.62O39E-01 5.2d680t-02PU-241 16 0.0 0.0 0 .0 0 .0PU-242 17 0.0 0 .0 0 .0 0 .0FISS C0UN1 91 0.0 0 .0 0 .0 0 .0
SUM 5 . 5 7 7 3 8 E - U 3 9.9U252E-01 ‘J.03548E-ol <i.623ft>£- 01
231
F IC T IC IO U S P L U T O H i V f EXFCSUREGIVtN A J J X t O S C U K C c1X2 GROl’ P, 2 POINTS STREAM OF C llA flU N CASES 13%NL tZ
SUMMARY OF NEUTRON LOSSES, ETC. BEFORE DEPLETING STfcP 1 UF CYCLE 1 T jtA L DEPLETION TIME j . o DAYS
ZONF CLASS EVERYB0D1ES
FISSILE0.11718
FERTILE 0.8810 7
INTERMEDiATt0 .0
CTKEP0 .0
STRUCTURAL SPECIAL UNSHtClFitO SLHS 0 .0 O.JOOOO 0 .0 U.9S623
CONV. rtATIO 7.36333
P O -cM fw )1 .o e^ 4 ifc -o »
F IS S Il ECkGI 3. V6ci43E-J«
— •» ______ OTHER LOSSES • BASEO CN START-CF-SIEP TOTAL LOSSES O.QC175 ___________OVERALL 0.11718 0.88107 C.C 0 .0 0 .0 0.00000 0 .0 1.00000 7.3eJ33 1.0S2t3E-03 3.96U43E-04
* ** w Aft M W T « n K 7 ;T * 6 TJffMIiTI ZTTTOK--------------------------------------------------------------------------------------------------------------------------------POWER NORMAL ItA T I ON 757.21333, MAXIMUM POM C R PENS 1TY 1.390137E 03 IN ZONE 1 AT END SUBSTEP 1
A ft fR STEP I OF CYCLE I t THE fIKE IS 20.0000 DAYS. THE TIME STEP WAS 20.0000 DAYS, ANU TOTAL TIME IS 20 .0000 DAYS
NUCLIOE REACTION RATES NORMAL 1 fEO TO 3.389258E 14 TOTAL LCSSES____________________________________ ________________________________________THE AMOUNT!KG> IS AT DEPLETION TIME 2.300000E 01 DAYS, AND THE REACTION RATES ARE AT DEPLETION TIME l.UOoOOOE 01 UAYS
TOTAL NUCLIDE REACTION KATES
N u C . AMOUNT ( K G > A d S O R P T l O N i C A P T U R E S P RO DU C T I O N SGRAPHITE___________________________ 5 1.19551E-03_______________________ 1.67915E-06 1.67915E-06 0 .0 ______________PU-239 14 3.7052 IE—04 1.132946-01 3.93570E-02 2 .0*5o0E-01PU-240_____________________________ 15 3.79356E-03_______________________t>.66482E-01 d.4dS39E-01 5.203bttE-02PU-241 16 1 .90893E-04 2.56974E-02 9.67U33E-03 4 .9o iy2E -02PU-242_____________________________ 17 2. 30833E-06_______________________7.1H290E-03 /.0b98BE-0:> 3.16445E-U6FISS COUNT 51 1.04782E-07 1.4&225E-X5 1.46225E-15 oTo
SUM 5 .55289E-03 1.0U555E 00 d.97647fc-0l 3.04239E-C1
FICTICIO U S PLUTOMIUH EXPCSURE GIVEN A FIXED SOURCEIX? GROUP* 2 POINTS STREAM OF CITATION CASES 1□RNL 72
SUMMARY OF NEUTRON LOSSES. ETC, FOR STEP 1 CYCLE I AT CYCLE DEPLETION TIME 10.00 DAYS. FISSILE KG IS AT 2 0 .Ou DAYS
ZONE CLASS EVERY RTDIES
FISSILE0.13899
FERTILE 0.86648
INTERMEDIATE CTHEP STRUCTURAL SPECIAL UNSPECIFIED 0 .0 0.00007 0 .0 0.00000 0 .0
SUMS1.00555
CONV. RATIO POftER(PU) 6.10496 1.23799E—03
FISSILEIKGI5.614I5E-Q4
_ _ _ _ _r __ OTHER LOSSES' BASED ON START-OF-STEP TOTAL LOSSES - 0.00555
OVERALL 0.11899 0.86648 f'.O 0.000C7 0 .0 0.00000 0 .0 1.00000 6.10496 1.23799E-03 5.61415E-04
TIME STEP THERMAL ENERGY. MW-HRS 5.94238E-01 AND TOTAL IS 5.94238E-01
NUCLIDF DFNSITIES BY ZONF ANO SUR-ZONE(NUCLIDE NUMBER - DENSITY) AT DEPLETION TIME 2 .OOOOOOE OIDAYS
ZONE NUMBER 1--EVERYBODISS5 '6 .M 0 & 0 F - 0 2 - 14 T . V T b l i t -T M 15"' S 7 T 1 S35 C-■03 16 4.77038E—04 17 5 .74463E—06 91 6.31052E-05
TIME STFP I REQUIRED 0.012 MI NUTES CPU TIME. AND' 01.143 MINUTES CLOCK TIME
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 1 CYCLE TIME 20.0000 DAYS TOTAL TIME 2C.OOOO DAYS
ITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3 DRIVE FACTOR BALANCE! 1 .19102E-01 1.00000 2 -4 .90379E-03 1.00000
0.2382 0 -0 .04608
-0 .18300 -0 .01256 -
0 . 00.00160
9.950700-019.951460-01
1.0049530.999924
3 -6 .508156-04 l.P^OPO4 -1 .008516-04 1.00000
0.12192 0. 16776
0.05739 0.36845
0.18121 0.14401
9.951730-019.951810-01
0.9999730.999992
-1 .2Z190E-05 1.30000 5112115 0.25001 0.t)73d4 9.951820-01 0.999999
END OP FIXED SO UR C FCA LCuLATIO N - 1TERATI Oto T I mF " £.560> MINUTES
LEAKAGE 575 TOTAL LOSSfS 3.68890fc 14 TOTAL PRODUCTIONS 1.18S90E 14 REACTOR POkEK(HATTSI 1.41006E 03
FICTICIOUS PLUTOMIUM EXPOSURE GIVEN A FIXED SOURCE__________________________1X2 GROUP. 2 POINTS STREAM OF CITATION CASES ORNL 72
GROUP T FLUX
1.5QOD 14
GROUP ? FLUX
12.154D 13
* * * WARNING HENRY, BftO NORMALIZATIONPOWER NORMALIZATION 50?.82813, MAXIMUM POWER DENSITY 2.0892fe5E 03 IN ZONE 1 AT END SUBSTEP
AFTER STEP 2 OF CYCLE 1, THE TIME IS 70.0000 DAYS. THE TIME STEP WAS 50.0000 OAYS, ANi) TOTAL TIME IS 70.0000 OAYS*****************■*****■*********-********************************************«************■*******
NUCLIDE REACTION RATES NORMALIZED TC 3.686899E 14 TOTAL LCSSESTHE AMOUNT CKGI IS AT DEPLETION TIME 7 .OOOOOOE 01 DAYS, AND THE REACTION RATES ARE AT OEPLETION TIME 4.5U00G0E 01 DAYS
roUO-p -
TCTAL NUCLIDE REACT ION RATES
AMOUNT(KG) 1 .19551E-03GRAPHITE
NUC.5
ABSORPTIONS1.40162E-06
CAPTURES1 . 4 0 1 6 2 E - 0 6
PRUDUCTIONS 0 . 0 ______________
PU -2 3 9PU-240
1415
3.122 30E-04 3.30851E-03
9.22391E—02 a.!38l4E-01
3.21312E—02 7.96339E—01
1.&4986E-015.06778E-02
°'J-241PU-242
1617
6 .19746E-04 2.59838E-05
9.tt7042E-02 9.00279E-04
3.68449E-028 . 8 5 9 6 0 E - 0 4
1.91764E—01 4.00941E-05
FISS COUNT 91 4.72755E—07SUM 5 .462 53E-03
8.08945E—15 1.00566E 00
8.08945E-1S8 . 6 6 2 0 3 E - 0 1
0 . 04.07467E-01
F IC T IC IO U S PLUTOMJUM EXFCSURE GIVEN A FIXfcD SOURCE__________________________1X2 GROUP, 2 POINTS STREAM Oh CITATIO N CASES QRNL 72
SUMMARY OF NEUTRCN LOSSES* ETC. FOR STEP 2 CYCLE 1 AT CYCLE DEPLETION TIME 45.00 DAYS. FISSILE KG IS AT 7C.00 DAYS
ZONE CLA55 FISSILE FERTILE INTERMEDIATE CTHEP STRUCTURAL SPECIAL UNSPECIFIED SUMS CQNV. RATIO POWER!PW1 FISSILE (KG )EVERVBOOIES 0.19094 0.81381 0 .0 0.0G090 0 .0 0.00000 0 .0 1.00566 4.17055 1.75449E—03 9 .32076E-04
OTHER LOSSES’ BASED CN START-CF-STEP TOTAL LOSSES --0 .00566 , M r x ± L _UverAll 0.19094 0.81381 0 .0 O.OOOSO 0 .0 O.OOQUO 0 .0 1.00000 4.17055 1.75449E—03 9 . 32076E-04
TIME STEP THERMAL ENERGY* MH-HRS 2.10539E PC AND TCTAL IS 2.69963E 00
NUCLIDE DENSITIES BY ZONE AND SUB-ZONEtNUCLIUE NUMBER - DENSITY! AT OEPLETIUN TIME 7.OODC00E OIOAYS
ZONE NUMBER 1— EVERYBOOI6S5 fc.ftAAWJE-62 14 T .a y ft jfc -O ii 15 8.30233E -03 16 1.54873F—03 17 6.46646E-05 91 2.84719E-04
t t d * ? REQUIRED 0.009 MINUTES CPU TIME, AND 0.150 MINUTES CLOCK TIME
tH t MICROSCOPIC CROSS SECTIONS IN SET 1 HAVE BEEN REPLACED BY THOSE IN SET 2
* FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE \ CYCLE TIME 70.0000 DAYa TOTAL TIME 70.0000 DAYS
ITERATION FLUX CHANGE BETA MU-1 MU-2 MU-3 DRIVE FACTOR BALANCE1 -1.65764E-012 4.48589E-02
1.000001.00000
-0 .33153-0 .22576
0.07869-0 .24169
0 .00.01353
1.045C8D 00 1.C4409D 00
0.9568631.000951
3 6.29902E-034 1.37520E-03
i . oooi’oI . 00000
6, 14672 0.21969
0.09S790.48160
0.237650.18673
1.043620 00 1.04344D 00
1.0004521.0001o9
5 2.14577E-046 -2 .92063E-0S
1.000001.00000
0.15625-0 .13614
0.37689 -0 .05691
0.0847U-0.13982
1.043410 UO1.043410 00
1.0000300.999995
END PF FIXED SOURCE CALCULATION - ITERATION TIME 0.000 MINUTES
LEAKAGE 0 .0 TOTAI LOSSFS 4.28731E 14 TOTAL PRODUCTIONS 1.7B7ME 14 RFAf.TOR POhERIWATTSI 2.06303E 03
235
PICT 1CIQ1 PLUTONIUM EXPOSURE GIVEN A FIXED SOURCE__________________________IX? GROUP, 2 POINTS STREAM OF CIT'.T.'ON CASES ORNL 72
6«OUP I FLUX
GROUP 2 FLUX
________ 1“ I 1 .7 9 ^ 0 13
*** WARNING HENRY, 640 K O H M A L I Z A T { O NPOWER NORMALIZATION 3 9 8 . 0 6 4 7 0 . MAXIMUM POWER D E NS IT Y 2 . 6 4 4 3 7 I E 03 IN ZONE 1 AT END SUBSTEP 1
“ z
111 STFP 3 OF CYCLE I t THE TIME I S 1 2 0 . 0 0 0 0 DAYS. THE TIME STEP WAS iO.OOOO DAYS, AND TOTAL TIHE IS 120.0000 DAYS
NUCLIDE REACTION RATES NORMALIZED TC 4 . 20 7 31 2 E 14 T CT AL LCSSEST h f AMOUNT(KGI I S AT DEPLETION TIME 1. 200000E O’ DAYS. AND THE REACTION RATES ARE AT DEPLETION TIME 9.S0U0C0E 01 DAYS
TOTAL NUCLiCF REACTION RATES
GRAPHITENUC. AMOUNT(KG)
5 1 . 1 9 5 5 1 E - 0 3ABSORPTIONS1.0059UE-06
CAPTURESl.C0590E-0o
PRODUCTICNS 0 .0
7 0 - 2 3 9P U -2 4 0
14 2.67483E-0415 2.77308E-03
6 . 1 1 3 8 6 E - 0 27 . 5 6 7 3 6 E - 0 1
2 . 1 3467E-02 7 . 33911E-01
1.0939 fE-01 6«<>1920E—02
PU-241PU- 24 2
16 1 . 0 3 3 2 1 E - 0 3 1? 6 . 7 4 0 2 4 E - 0 5
1.5!>592E-012.t>247db-03
5 . 76351E-02 2.4d43*E-d3
3 . 03668E-01 1 . 13277E-0*#
H s s COUNT 91 9 . 6 5 9 4 7 E - 0 7 SUM 3 . 3 3 7 6 4 E - 0 3
1 . 0 8 9 B 8 E - 1 49 . 7 5 9 9 3 c - 0 1
1 . 6 8 9 8 8 E - 1 H8 . 1 5 3 7 8 E - 0 1
0 .04 . 793 70E-01
F IC T IC IO U S PLUTOMIUM'EXFCSURE GIVEN A FIXED SOURCE1X2 GROUP, 2 POINTS STREArt OF C I T A T I O N CASES 1DRNL 72
Su m mAr y OF NEUTRON LOSSES, E T C . FOR STEP 3 CYCLE 1 AT CYCLE CEPLETION TIME 9 5 .CO DAYS. i l S S I L E KG I S AT 1 2 0 .0 0 DAYS
ZONF CLASSe v e r v b o o i e s
F I S S I L E0*21673
F E R TILE 0 .7 5 6 7 4
INTERM EDIATE OTHER STRUCTURAL SPECIAL UN S PEC IFIED 0 . 0 0 .0 0 2 5 2 0 . 0 0 .0 0 0 0 0 0 .0 0 0 0 0
SUMS 0 .9 7 5 9 9
CCNV. R A TIO POWEK(FH) 3 .3 8 6 2 7 2 .3 5 7 1 B E -0 3
F I S S l L E ( K b ) 1 .3 0 0 6 9 E —03
OTHER LO S S ES ' BASED CN S T A R T -C F -S T E P TOTAL LOSSES 0 .0 2 4 0 1
flvf^ALL 0 .2 1 6 7 3 0 .7 5 6 7 4 0 . 0 0*00252 0 . 0 0 .0 0 0 0 0 0 .0 0 0 0 0 1.0 0 0 0 0 3.381)27 2 .3 5 7 1 8 E -0 3 1 .3 0 0 6 9 E -0 3
T IM E STFP THERMAL ENERGY. MW-HRS 2 .8 2 8 6 2 E OO ANb TOTAL IS 5 .5 2 8 2 4 E OO
N U C L !06 D E N S IT IE S RY ZONE AND SUB-ZO N E(N U C LID E NUMBER - D E N S IT Y I AT OEPLETION TIME 1 .2 0 0 0 0 0 E 020AYS
ZONE NUMBER 1— EVERVBOOIES5 6*000001:— 02 14 6 .7 4 0 27F.-04 15 6 .9 5 8 7 5 E - 0 3 16 2 .5 8 1 9 6 E —03 17 1 .6 7 7 4 1 E -0 4 91 5 .8 1 7 4 5 E -0 4
TIM ? Ste*> i ttEQutREB O .O iO MINUTES CPU T I M E , AND 0 .1 5 7 MINUTES CLOCK T IN E
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOK CYCLE 1 CYCLE TIM E 120.0000 CAYS TOTAL TIME 1 2 0 .0 0 0 0 DAYS
IT E R A T IO N FLUX CHANGE BETA MU-1 M U -2 MU-3 ORIVE FACTOR BALANCE1 2 .6 4 3 5 3 E -0 12 - 7 . 2 9 9 3 0 E - 0 2
1 .0 0 0 0 01*00000
0.52871-0 .3 4 9 1 1
- 0 . 2 6 9 3 2 - 0 . 0 8 6 8 9 '
0 . 0-0 .0 1 8 7 0
9 .2 6 5 7 6 D -0 19 .2 8 4 5 1 0 -0 1
1 .0 7 9 2 4 20 .9 9 7 9 B1
3 - 1 . 0 5 6 1 2 E - 0 24 - 3 . 1 8 8 6 I E - 0 3
1 .0 0 0 0 01 .0 0 0 0 0
6 .1 3 4 1 30 .2 9 8 7 3
0 .1 4 6 5 50 .6 5 5 9 1
0 .3 2 3 0 40 .2 5 8 7 0
9 .2 9 6 6 2 0 -0 19 .3 0 2 8 9 0 -0 1
0*9986970 .9 9 9 3 2 6
- 6 . 9 3 0 Z 3 E - 0 4 6 1*73569 E -0 4
1*066661 .0 0 0 0 0
0 .2 1 6 6 5-0 .2 5 0 2 8
0 .5 2 1 5 3- 0 . 0 8 2 8 5
0 .1 3 0 2 4-0 * 1 2 6 3 4
9 .3 0 4 5 2 0 -0 1 9 .3 0 4 2 6 0 -0 1
0 .9 9 9 B 2 51 .0 0 0 0 2 8
1 - i * ? 1 T S 2 F -fi¥ i .d o o n o - 0 .1 5 9 7 1 - 0 .0 6 9 1 1 - P . 25863 9 .3 0 4 3 3 0 -0 1 0 .9 9 9 9 9 3
END .bfc FlJteO SOURCE C ALCULAtlON - I T E R A T IO N TIME C .O O l MINUSES
LEAKAGE “577 TOTAL Losses 5.1*227E 14 TdtAL rtOO UCfiO N i 2.62227E 14 REACTOR POxEKIWATTS! 2.99171E 03
FICTICIO US PLUTOMIUM EXPOSURE GIVEN A FIXfcU SOURCE__________________________IX ?. GROUP, 2 POINTS STREAM OF CITATION CASES ORNL 72
GROUP 1 FLUX
11 2 . 0 2 6 0 14
GROUP 2 FLUX
_______ 11 1.5550 13
» * * WARMING HENRY, BAD NORMAL H A tlO N>0WER NORMALIZATION 295.69141, MAXIMUM POWER DENSITY ,3»559B9'»E 03 IN ZONE 1 AT END SUBSTEP 1
AFTFR STEP 4 OF CYCLF I , THE TIME IS 170.0000 OAYS. THE TIME STEP VJAS 50.0000 DAYS* AND TOTAL TIME IS 170.0000 DAYS
NUCLIDF REACTION RATES NORMALIZFD TO 5.122267E 14 TOTAL LCSSESTHE AMOUNTUGI IS AT DEPLETION TIME 1.700000E 02 OAYS, ANO THE REACTION RATES ARE AT DEPLETION TIME 1.4S0000E 02 DAYS
TOTAL NUCLIDE REACTION RATES
GRAPHITENUC.5
AMOUNT(KG) 1.19551E—03
'.SORPTIONS7.28816E-07
CAPTURES7.28816E-07
PRODUCT IONS 0 . 0
PU-239PU-240
1415
2.25164E—04 2.1871SE—03
4.B3107E-02 6.93152E-01
1.69658E-02 6 . 71499E—01
8.65217E-026.27944E-02
PU-241PU-242
1617
1.4205CE-031.29982E-04
2.09519E-015.97804E-03
7.60464E-02 5.88C89E—03
4 .13764E-01 2.72014E—04
FISS COUNT 91 1.65045E-06 3.35555E-14 3.35555E-14 0 .0SUM 5 .1 5999E—03 9.56960E-01 7.70392E-01 5.63352E-01
F IC TIC IO U S PLUTOMIUH EXFCSURE GIVEN A FIXED SOURCE1X2 GROUP, ? POINTS STREAM OF C I T A T I O N CASES ORNL 72
SUMMARY OF NEUTRON LOSSES , E T C . FOR STEP 4 CYCLE 1 AT CYCLE DEPLETION TIME 1 4 5 .0 0 OAYS. F I S S I L E KG IS AT 17C.OO OAYS
ZONF CLASS F I S S I L E F E R TIL E INTERMEDIATE OTHER STRUCTURAL SPECIAL UNSPEC IFIED SUMS CGNV. RATIO POriERtPM) F I S S I L E ( K G )EVERYBODIES 0.2 5 7 8 3 0 .6 9 3 1 5 0 .0 0 .0 0 5 9 8 0 . 0 0 .0 0 0 0 0 0 .0 0 0 0 0 0 .9 5696 2 .6 0 4 4 3 3 .2 8 0 J 9 E -0 3 1 .6 4 5 6 7 E -0 3
OTHER LOSSES* BASEC CN S T A R T -C F -S T E P TOTAL LOSSES 0 .0 4 3 0 4 _______OVERALL 0 .2 5 7 8 3 t i .69315 O . f 0 .0 0 5 S B 0 . 0 0 .0 0 0 0 0 O.OOUOO 1 .0 0 0 0 0 2 .6 0 4 4 3 3 .2 U 0 3 9 E -0 3 1 . C4567E-03
T IM E SfEP THERMAL ENERGY, MW-HRS 3793647E 00 AND TOTAL IS 9 .4 6 4 7 1 E 00
NUCLIDE D E N S IT IE S BY ZONE AND SUB-Z0NECNUCL1DE NUMBER - D E N S IT Y ) AT DEPLETION T IM E 1.700000E 02UAYS
ZONE NUMBER 1— EVERYBOOIES5 6 .0 0 0 0 0 E -0 2 14 5 . 67388E—04 15 5 .4 & 8 5 1 E -0 3 16 3 .5 4 9 8 0 E -0 3 17 3 .2 3 4 8 1 E— 04 91 9 .9 3 9 9 1 E—04
TIM E SfEP 4 REQUIRED 0 .6 1 0 MINUTES CPU T I ME « AM) 0 .1 6 6 MINUTES CLOCK TIME
A FIN AL FLUX - EIGENVALUE PROBLEM ITE R A T IO N FLUX CHANGE BETA
FOLLOWS FOR CYCLE MU-1 MU-2
1 TOTAL DEPLETION TIME MU-3 DRIVE FACTOR
1 7 0 .0 0 0 DAYS BALANCE
1 2 .7 1 6 8 6 E -0 12 - 1 . 6 3 5 5 9 E - 0 1
1 .0 0 0 0 0 i . 00000
0 .5 4 3 3 8 - 0 . 76557
-0 .2 0 5 1 3- 0 . 2 2 0 8 5
C .O-0 . 0 3 1 1 2
8 .3 5 1 5 6 0 -0 18 .3 9 5 8 8 0 -0 1
1 .1 9 7 3 8 00 .9 9 4 7 2 1
3 -2 .0 5 1 9 3 E - 0 24 - 8 . 394 5 4 E-0 3
1 .0 0 0 0 0 1.0 0 0 0 0
0 .1 0 4 9 4 0 .40071
0 .2 0 6 8 6 0 .8 8 2 1 9
0 .4 3 3 3 20 .3 5 5 3 0
8 .4 3 4 2 9 0 —01 8 .4 6 1 5 9 D -0 1
0 .9 9 5 4 4 60 .9 9 6 7 7 4
5 3 .1 9 0 0 4 E -0 36 1 .2 7 2 2 0 E -0 3
l.oooec1 .0 0 0 0 0
-0 .3 7 6 8 2 0 .4 0 0 0 8
- 0 . 5 6 5 6 80 .1 2 1 7 8
0 .1 9 9 2 8-0 . 1 1 2 7 3
8 .4 7 2 4 6 D -0 1 8.4 7093D—01
0 .9 9 3 7 1 61.0 0 0 1 8 0
1 — 1 .7 9 1 V2E—64 8 4 .7 6 8 3 7 E -0 5
1 .0 0 0 0 3i.OCOOC
- 6 . 14101 ~ C . 26609
- 0 . 0 7 4 4 2 — 0 .2 7 6 G 5
-0 .2 6 8 9 3-0 . 2 6 8 2 0
8 .4 7 1 3 4 D -0 18 .4 7 1 2 3 D -0 1
0.9 9 9 9 5 11.00 0 0 1 2
9 — 1.28150E—05 1.0 0 0 0 0 -0 .2 6 8 7 6 - 0 . 1 5 0 S 4 - 0 .2 6 4 2 1 8.47126D —01 0 .9 9 9 9 9 6
END OF F IX ED SOURCE CALCULATION - I T t R A t l O N TIME 0 .0 0 1 MINUTES
LEAKAGE 5775 TOTAL LOSSES 5 755T35TTT? t6TAL PRliDUCtlONS 3.99156E 14 REACTOR PUWERIMATTSI 4 . 5231) IE 03
239
FICTICIOUS PLUTONIUM EXPOSURE GIVEN A FIXED SOURCE__________________________IX? GROUP, 2 POINTS STREAM OF C ITATION CASES OKNL 12
GROUP 2 FI U*
_______11 l . w o o I f
FINAL NUCCtOF REACTION HATES FOR CYCLE I TOTAL DEPLETION TIME 170.00 DAYS
TGTAL NUCL1CE REACTION RATES
NUC. AMOUNT(KG) ABSORPTIONS CAPTURES . PRODUCTIONSGRAPHITE 5 1.19551E-03 5.1669UE-07 5.I6698E—07 U.OJHJ-239 1* 2.25164E-04 4.3B914E-02 1.5bOB8E-Q2 7.86790E-02PU-240 IS 2 .1 8 7 19E-03 7.10162E-01 6.87409E—01 6.59823E—02PU-241 16 1.42050E-03 2.34967E-01 8.34172E-02 4.69803E—01PU-242 17 1.29982E-04 9.16891E-03 9.C1842E—03 4.21382E-04F IS S COUNT 91 1.65045E-06 4.83837E-14 4.83837E-14 0 .0
SUM 5.159S9E-03 9.9S189E-01 7.95349E—01 6.148U6E-01
FIC T IC IO U S PLUTOMIUH EXPOSURE GIVEN A FIXED SOURCE1X2 GROUP. 2 POINTS STREAM OF CITATION CASES ORNL 72
FINAL SUMMARY‘ OF NEUTRON LOSSES, ETC. FOK CYCLE 1 TOTAL DEPLETICN TIME 170*00 DAYS
ZONE CLASS EVERYBODIES
FISSILE0.27886
FERTILE INTERMEDIATE OTHER SIRUCTURAL SPECIAL UNSPECIFIED SUMS CONV. RATIO 0.71016 0 .0 0.00917 0 .0 0.00000 O.OOCOC 0.99819 2.4o308
POWER 1 PH) 4.52350E-03
FISSILE (KG ) 1 .64bo7E-03
_, ____ OTHER LOSSES' BASED CN START-CF-STEP TOTAL LOSSES 0.0C181
DvEfcALL 0.27886 C .71016 0 .0 0.00917 0 .0 0.00000 O.OOOCO 1.00000 2.46508 V.52350E-03 l.£<r5o7E-03
CVCl E ! REQUIREO 0.050 MINUTES CPU TIME « ANO 0.32b P I MITES CLOCK TIME
MICROSCOPIC CROSS SECTIONS HAVE BEEN RETURNED TO THE ORIGIONAL SPECIFICATIONS
FICTICIOUS OLUTUMIUM e x p o s u r e g i v e n a f i x e d s o u k c e1X2 r.POUP, ? POINTS STREAM OF C I T A T I O N CASES ORNL 72
A H lIX - FIRfNVALUE PROBLEM FOLLOWS FCK CYCLE 2 CYCLE TIME 17 0. 00 00 DAYS TOTAL TIME 17C.0000 OAYS
l i n f r e la x a t io n w i l l b f done tn rows - 1 inner i t e r a t i o n i s iITERATION FLUX CHANGE 8EIA HU-1 HU-2 MU-3
1 -9 .93629E -C 1 1 .Of 000 -1 .98726 0 .0 0 .0K
0.5504032 b .b 1.00000 0 .0 0 .0 O.OOUOO3 0 .0 1.00000 0 .0 0 .0 l.QOOOO
0 . 5 5 0 40 50.55041)5
ENn OF EItifNVALUE CALCULATION - 1TFRATION TIHE P.COO MINUTES
CONVERGFHCE INOICATION HY MINIMIZING THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 0.9999999 K 0 .5 504049
11 AKA OF 0 .0 TOTAL LOSSES 1.68964E IS TOTAL PROUUCTCZjNS 9.29986c 14 REACTOR POhER(WATTS) 1.05263E 04
ro-fr-ro
PICT TC TOIJS PLUTflMIUM FXPOSURC GIVFN ft FIXED SOURCE__________________________1X2 GBHUP, 2 POINTS STREAM OF CITATION CASES ORNl 72
CROUP 1 FLUX
11 i .O l lD 15
GROUP 2 FLUX
_______ 11 "4.924D l i
NUCLIDE Pf4CTinw RATES NORMAL 17fD TO 1.609639E 11> TOTAL LCSSES THF AMOUNTI KG) IS AT DEPLETION TIME 1.700CQ0E 02 OAYS. AND THE REACTION RATES ARE AT DEPLETION TIME 1.450UQ0E 02 DAYS
TOTAL NUCLIDE REACTION RATES.
NUC. AMOUNT(KG) ABSORPTIONS CAPTURES PRODUCT IONSGr a p h it e 5 1.195&1E-03 5.57305E-09 3.57305E-09 0 .0PU-239 14 2 .2 5 1 64E-04 4.0U562E-02 1.46377E-02 7.34031E-02PU-240 15 2.1871SE-03 7.40664E-01 7.22154E—01 5.36765E—02PU-2-41 16 1.42050E—03 2.04655E-01 6 . 02733E-Q2 4.22784E-01PU-242 17 1.29982E-04 1.16105E-02 1.14170E-02 5«41752E—04FISS COUNT 91 i.65045E -06 5.94765E-14 5.94765E-14 0 .0
SUM 5.159S9E-03 9.977U5E-01 8.16482E-01 & ,50405E-0l
H t f i c i t y j s P iu io » t u » t * u s u « i * M «*t> sojK CtI s ? i iv n g p , i P d i M S SlRfAM u f U t A l l t J * CAifcS UHNl 72
smhmA&y nF SffutKi*< PU t lf#t ill*1 Jo* iYcT? 5 ftital ott'tiuo^ u rn T7u7ou~ua7> :
'C l*SY” “*FTS*>l i r y ffc lilt I *ff * Mta’I a 11 cTnl F -! lauc! ukal~$»>£Cl*l uNifpTc f f l fc'si itS s ' ccnvVVat7u PU*iM>*) n SSlLi { Kl>*CVM fM OIfS a.2«S*l C. HQbb C.O C .O H M 0 .0 o,000(» J . J j .V W fv 2.VhU1 1. JicoiE-U.? 1. *».:>& 7fc-j 3
-----------------------------------------------------------------------— - f t T ^ T r T E v s n t m i m ch 's ^ .wt - c T T r r i P- r d t k i o SA s ~ u c f i i ----------------------------------------------------------------- -----------------
- " w r w n . ” ' T 3 W * n . ,R W T " " " ■ v . m u i * . r - e .a w w o.b l.OUuUO 2.44143 I.OS263E-02 1, Mott-03
H M (> «OK*A|t.ATION * «H 3 7 ? "» NAXIMU* PUMtH OtKSITY 1 .2$6 »7£ t C4 1* /0».E 1 Af ENU SUnSIEP 1
^4 < lfp f rV t¥2» t >* tot H c .c c e c C*YS. !m£ lik s S?ti» MAS 30.9090 OAYS, ANU IU1AL r ix i IS 2U.J.0U00 'JAYS
NUCLIDE BMC HON RATES <snftrtAL l/ r » If. I.bft*b19t 15 TOIAj. LCSiESIMF MOUHTtKGl 13 AT rtfPL fllC W TIMS ?*ilOOUOUt 02 OAYS* ANt, TW£ K iAU IO N H A lt i AKt A| O fPLH IU N 1 life l. i'jO O Q u i 02 UAYS
m m j Cl ic £ Kfci'CTTuh K A T t i
GJUPHITE■ v g = m —
P U - 2 4 0 ___p u -2 * :P U -2 4 2
iss tnuH i
r o . " " gftpgx m g i "
1 .6 4 2 « 3 F B + '
c a p t u r e sj>.573USL-U9
PRODUCTIONS 0.0_______ _
1*IS 1.227+35-0316IT*r
SUM
1.93*B4f-032.»6fc«2E-0*3.0V4O9E-J64 .7 7 2 d if -n »
AbSOHPtluNS >.& 73ot>£-09 3.»i3C*t-026.217C3I--01_______________2 .+ 1 7 ? d c -O l « .0 6 i7 ? fc -U 2 4 .9 * 4 / 4 1 -0 11.6 t t l9 d t -0 2 i.b !»3 q i> E -0 2 7 .t t ia 2 2 1 -0 4
1 .2 o 5 « 2 t - C 2fa .0t»l68E-01
6 .3 4 7o4£-C2 4.:>0:>64E-0 2
ro■P”-Pr
a .s + o ttjc -4.1*634t-
u01 7.1b024E-01
0 .0O .0 o 7 * 2 t -0 l
FICTICIO U S PLUTONIUM EXFCSURE GIVEN A F1XEO SOUKCE1X2 GROUP. 2 POINTS STREAM OF CITATION CASES ORNL 72
SUMMARY OF HfeutRGN LOSSES, ETC. FUR STEP I CYCLE 2 AT CYCLE OEPLETION TIME la i.O O DAYS. FISSILE KG IS AT 20C.00 OAYS
ZONE CLASS FISSILE FERTILE INTERMEDIATE OTHER STRUCTURAL SPECIAL UNSPECIFIED SUHS CCNV. RATIO POwkRIf'k) FISSILE (KG )E VERY 6001ES 0.27711 0.62171 0 .0 ____ 0.01682 0 .0 _____ 0.00000 0 .0_____ 0.91563 2.16747 1.1607*E-Q2 2.10011E-03
OTHER LOSSES* BASED CN START-CF-STEP TOTAL LOSSES 0.06437
OVERALL 0.27711 0.62171 OTO : 0 .01682 O 0.00000 0 .0 I . 00000 2.18747 1.16U74E-02 2.1U011E-U3
TIME STEP THERMAL ENEPGV, NW-HRS 8T35734E 00 ANO TOTAL IS 1.78221E 01 ' " ' '
NUCLIDE DENSITIES BY ZONE ANO SUB-/ONE(NUCLIDE NUMCEK - OENSITYI AT DEPLETION TIME 2.00U00UE 02DAYS
ZONE NUMBER 1 --E V E R Y BODIES ................... ......................................................................................................................................................................5 6 . 66606E-0 2 R 4.139246-04 T5 3 .6a024 t-0J 15 4.83764E—03 17 6.137>dE-04 51 1.86343E-03
TIME STEP I REQUIRED O.OlO MINutES CPU TIME. ANO 0.156 MINUTES CLOCK TIME
A flU X - EIGENVALUE PROBLEM FOLLOWS FOK CYCLE 2 CYCLE tlME 20C.OOOO DAYS TOTAL TIME 200.0000 OAYS
ITERATION FLUX CHANGE BETA MU-1 H U -2 H U -3________________ K_____________________________________________________________________1 - 2 . 7 1 1 1 5 E - 0 1 1 . 0 0 0 0 0 - 0 . 5 4 2 2 3 OTO 57o 0 . 8 1 10 4 2 2_______ <M )______________ 1 .0 0 0 0 0 0 .0 _________C M )__________ 0 .0 0 0 0 0 ________ 0 .8 1 1 0 4 2 ________________________________________________________________3 OTO 1.00000 OTO OTO 1.00000 0.811042
H B OF E1CENVALUE CM-CULA NON - 1 TERfl f lT W T I HE ""O'. ft------STITJUTFS---------------------------------------------------------------------------------------------------------------------------
tcilVERGENtfe iNOICAtlrtN BY MINIMIZING THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 0.999949V K 0.6110417
LEAKAGE OTS TOTAL LOSSES 1.15311E 15 toTAL PRODUCTIONS 9.35224E 14 REACTOR POWER( WATTS) 1.C526 3E 04
F1CTICIHUS PLUT0M1UM EXPOSURE G1VFM A FIXED SOURCE__________________________1X2 GROUP, 2 POINTS STREAM UF CITATION CASES ORNL 72
GROUP 1 FLUX
1i a.Aron 14
GROUP 2 FLUX
_________J ______I 2 .9 3 0 D i f
POWER NORMALI7A1ION 0 .9 9 8 5 9 , MAXIMUM POWER D E N S ITY 1 .0 5 4 1 2 1 E 04 IN 2CNE 1 AT END SUBSTEP 1
AFTER STFP 2 OF CYCLF 2 , THE T IK E IS 2 3 0 .0 0 0 0 CAYS. THE TIM E STEP WAS 3 0 .0 0 0 0 OAYS, AND TU TAL TIM E IS 2 5 0 .0 0 0 0 DAYS
N UCLIDE REACTION RATES NORMALIZED TC I.1 5 3 1 1 5 E 15 T C T A l LCSSES____________________________________________________________________________T H E AMOUNT IKGI I S' 4 T D E P L E T I O N flME 2 . 3 0 0 0 0 0 E 0 2 O A Y S , AND THE R E A C T I O N R A T E S ARE A T DEPLETION TIME 2 . 1 5 U 3 0 0 E 02 D A Y S
---- rtmtrUnTLlDETiTAdTIffNNUC. amOu n t ( k 6I ABSQRPTIUNS CAPTURES PHQOUCIIQNS
GRAPHITE 5 1 .1 9 5 5 1 E -0 3 6 .0 9 8 U E -0 9 6 .0 9 8 1 2 E -U 9 0 .0P U -2 3 9 14 1 .2 6 3 9 6 E -0 4 3 .2 1 0 7 o 6 -0 2 1 .1 5 0 3 5 E -0 2 S .7 6 8 S 2 E -0 2P U -2 4 0 15 6 .9 9 5 1 2 E -0 4 4 .9 4 8 0 2 E -0 J 4 .B 2 4 3 5 E -C X 3.iJ8t>21fc-02W -2 4 1 16 2 .0 3 ^ 1 l E -O i 3 .4 8 2 6 1 ^ -0 1 1 .1 6 1 7 1 E -Q 1 7 .1 9 4 7 9 E— 01P U -2 4 2 17 3 .4 7 7 7 2 E -0 4 3 .2 3 3 2 7 E -0 2 3 . 1 7938E-02 1 .5 0 8 6 U E -0 3 ,F IS S COUNT 9 t 4 .4 0 B ? 3 E -0 6 1 .6 4 6 4 U E -1 3 1 .6 4 6 4 8 E -1 3 0 ,0
SUM 4 .4 0 8 7 5 E-0 3 9 .0 7 5 0 3 E -0 1 6 .4 1 9 0 4 E -0 1 8.14!>35E-01
2k6
F IC T IC IO U S PLUTOftlUH EXFCSURE G IVEft A F IX E D SGUkCfc1X2 CPOUP, 2 P O IN TS STREAM OF C IT A T IO N C A S tS ORNL 72
SUfMABY O f NEUTRON LOSSES*I e t t . FOR STEP 2 CYCLE 2 AT CYCLE C E P LE IIO N TIM E 2 1 5 .0 0 WAVS. F IS S IL E <6 I S AT 2 3 0 .0 0 DAVS
20NF CLASS EV c»YB O D IES
F I S S I L r0 .3 8 0 * ?
F E R T IL E0 .4 9 4 B 0
IN TEK M H )IA T£ C T H td STRUCTURAL SPEC M L M S P i t l F l E O G .O 0 .0 3 2 2 2 0 .0 0 .0 0 0 0 0 0 .0
SUMS0.9Q 75C
COftV. R A T IO 1 .2 6 * 3 4
P O h E H t f h l1.05C .08E-02
F IS S IL E IK G J 2 . 16151E-03
ww _Wf|T1_ 01H£R LO S SFi* BAS«rC CN S T A R T -C F -S T E P TO TAL LOSSES 0 .0 9 2 * 0
fivf M i l ... O . i t e t f 0 .4 9 4 ^ 6 0 .0 0 .0 3 2 3 3 2 .0 0 .0 0 0 0 0 0 .0 1 .0 0 0 0 0 1 .2 6 0 3 + 1 .0 5 O C B E -0 2 2 .1 6 1 5 1 5 -0 3
TIM * STFP THERMAL LN£R&Y* MW-•tiki 7 .b r 3 7 t £ t C AKD TOTAL IS 2 .5 * 2 5 u E 01
f f l J t ' C T f c E “ F tT N s 'A w S u tw u N E tN u tu u f c number - d e n s i t y } a t bifrifclUtm l i n t 2\3otsooot 020 a y s
1 0 M w w n J — EVEB V ^nD IES ------------5“ S733(J33F=o?---------------------l-v j.leia^t-o* ..lt> I . f* imJf-oi \u ±.u6*tii-u3 Y> a.b>*$5i-c+m r o ^ r u R iP T O '- vr.w*?«nrrs •cvyTW^ANb" -o. vsr hikju* Hat*, r i « t ------------------------
V I 2 .6 * > m - i> 3
a t tn > t~ y t u u - ~ n f i t H v m i F M Tire f H f i H A J i i r y e n r r v u i i i d U t d t f r i M i B i m i H tI T J R M J P N FLUX CHANI*F HFTA H U-1 M U-2 M U -3 it“ — r — m — h t b t s s — o T v i & r c — 37o---------------- s r s --------------------------n a a n s
? 0 .0 1 .0 0 9 0 0 0 .0 0 .0 C .0 0 0 0 P l.OOfcfl?* 0V0 ” ■-— ■ -* . ,uggoS"" V. „ -— 0vg- ------- IVftTomj-------“ K B O TTgfcg" o » h b w i c w em e n m l o w - " t t h u t i b t i m ' ~ B .W 3 ~* i* u re i ........... "........... —
2 3 C .0 0 0 UATS
t i w y r g g m r m r i u r k i w s g w i y p i m w , M f w i ut ~ i* e s w i m s > / t o t w t n c u t i - * i a t i v t ; * » s & d n i u » r o . v v H v w
- "XT SkSM 5.~b.............
ro* r-4
K 1.0C8«2:>3
IONS 9 , JJ1 6 0 C I t KSACtfct * W R ( K * f T S l U 0 » 2 * 3 £ 04
n c n c ir w s m m m w * c epusuwe GivfN t k » i p sounci ___________________" i«? cutup* t *oi«iis si**** up ciuiitM cams uism. «
tiki*}? fTEuS"
W H IP 2 f lU X
I i i
P t m t H U C tiB f W CACftflll WftTfS C V C tf 2 I 0 I U C t K C f l O H t m t i i O . J O OATS
l O l M W C l i e i i t i K H i a naffcS
M U C . A M C t l k l l K C I A t t S U a P I I t i U G l u t e i c K d d y m u t t
& « P | t l I E * r . « % o - » k - c ^ o . c
P l l - 2 9 9 u i . 2 6 3 < i * E - 0 4 3 . 4 4 b i t t t - u 2 I . J H W J - W * . l « 2 / ? t - t £ ......
^ U ' W O i i 4 . 6 3 0 0 2 1 - 0 1 1 . 4 4 1 I 4 E - C 2
« » - 2 4 l 1 6 2 . 0 3 5 1 1 C - 0 3 4 . 4 U t > i 2 £ - 0 l l . 4 * « * 6 f - 0 I 9 . 1 0 J 0 U - 0 1
^ u * w i .......... ..... i 1 2 . i ? < « * t - 0 }
f i s s c a u * t V I 4 c * 0 t 7 3 1 - 0 6 2 . J S t t * f - t i u . J . . . .__
* y * 6 . 6 « z r « - 0 l l . U u M i t 0 0
CP
F IC T IC IO U S PLUlCH lUW M FCS UR E G IVEN A FlX EO SOURCEi » ? gro up* 2 ?oi*rs s tk e a h op c i t a t i o n c a s e s o m 72
P in a l summary at- n e u tro k ld & s c s , t V c . IstK cvcife 2 to V a l c ^ L f i r i o * t t itE 2 *0 .0 0 b a y s
ZOKF CLASS EV5R YB30IFS
F IS S IL E F t R T H c IV ttR M tO IA T F OTHER STRUCTURAL SPECIAL (JhSPECIFIfcO SU8S 3 .4 T S IP 0 .4 7 4 8 7 0 .0 0 .0 4 6 7 0 O .O U . 00000 0 .0 0 .V V 6 6 7
CCftV. R A TIO POnfcfclPttlI .O S 2 6 3 E -0 2
F IS S IL fc lK C I2 . l * l S » E -0 3
UlrtFR LOSSES* 8ASEC CN £ lA * l -C I -> S t E » tO TA L LOSSES O .0C333 ,_ru, , „O V t t A l l C . i / i t f * t .V jf t 8 7 f . C 6.<!>467C 0 .0 0 .0 0 0 0 0 0 .0 l.O O U O C 0 .4 7 * 3 4 1 .0 S 2 6 3 E -0 2 2 .1 6 l > I E -0 3
C Y C lf ? "EOUIRKO 6 .C S 5 m j NUTf s CPU TIM E* AND 0 .4 3 0 N U U IE S CLOCK 1 ! «
EMS ffp C i'S T - l O H L f l**P C . i 5 M ftU ff& I O U l C l OCR I I m£ MA£ | . 0 * I t U u ^
« • • * • • • # * i M K i J O B ni,S RUN ON O H r ^ CN ThE IBM 360.
MULT I -C Y C L E W EEPER ISMEARED RODS *0JU S T E D , RECYCLE FEED DETERMINED!1 & M 3 <i«OUPS? Z6S PO IN TS tR -Z > . STREAM OF C IT A T IO N CASES ORNL 72
"m ic ro s c o m c r o s s -s c c n o * u P & * rito i f c u o w t
«***»**e<jNTMi option r r *******------------
MEM CROSS iE C t lO N TAPE 8 MADE
UlCftCSCOPiC CRB55-5eCTTffH TiTCgrrW PPLLOwS
4**u**tmRou~i>mw r r ------------
CWT55 SECTT O T 5ET 'iMBEP"T O T O F f f
M lftld&COPlC C R O S S -S E C t lON UPDATING FOLLOWS
gHiEK K t m m r m t n -T t c n oiraffi------------------------------------------------------------
I C 0 5 S S 0 S IT ~ 0 Q 0 3 9“ 9 0 0 0 0 0 0 0 o 01 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
itio 100 H! 2 5 9 9 5 9 5 9 5 9 9 9 8 5 o' 5 * 12 s 12 isl.OOOOOOE 01 1 .0 0 0 0 0 0 E -0 5 9 .9 9 9 9 9 9 E 09 9 .9 9 9 9 9 9 E 23 0 .0 _______________ 1 .OOOOOOE 00________________
D EP LETIO N HISTORY IN PU T - SECTIO N 002
3 2 2 2 1 0 0 0 1 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0S.fcOOOME 03 i.S O O O O fe 03 57o 1 .OOOOOOE 00 — 5 .OQOOOOE-01 1 .OOOOOOE 007 .5 0 0 0 0 0 E 01 7 .5 0 0 0 0 0 E 01 7 .5 0 0 0 0 0 E 01 7 .5 0 0 0 0 0 E 01 7 .5 0 0 0 0 0 E 01 7 .500000E 01“ 9 6 9 9 *1 9 9 9 9 9 0 9 9 9 9 9 9 0 0 0 0 0 0 0
WEgTWOW T IP * MOBLEH HgSCM m O N - ' SECTION"003---------------------------------------------------------------------------------------------------------
9 I 9 9 7 0 0 0 0 0 I 9 9 I 9 9 9 9 9 9 9 3 0 09 .9 9 9 9 9 9 E -0 5 1 .0 0 0 0 0 C E -0 9 9 .9 9 9 9 9 9 E -0 5 9 .9 9 9 9 9 9 E -0 5 9 «9 9 9 9 9 9 E -0 5 0 .0570------------------------070---------------------?7S90000E *03' ~"97 7U0IT0DE-01 ^.000909^-01 3 .0 ----------------------------------------------
lE ^ i iT S P | A it iH i| B D T t d N ^ M n iT | {X C K BOUNDARY c o N o m b ^ ARt0 .0 _______________* .6 9 2 0 0 0 6 -0 1 + .6 9 2 0 0 0 E -0 1 ___0 .0 ______ 4 .6 9 2 0 0 0 E -0 1 ___4.& 92Q Q 0E-01
TWO DIMENSIONAL C Y LIN D R IC A L GEOMETRY |R , 2 »___WIOTH 2 .1 3 9 9 9 9 6 02 H EIGH T U lO O O O O E 02
REGION S P E C IF IC A TIO N S
250
P TS KEttlON N IO TH2 9 .1 2 3 1 3 0 6 01 2 3 .7 7 8 4 7 0 E 01 2 2 .6 9 9 3 9 9 6 01 2 1 .3 4 9 3 4 0 E 01 2 I . 25066OE 01 2 3 .0 0 0 0 0 0 E 01
PTS REGION HEIGHTi 3 .o o o 66o e o i 1 1 .8 0 0 0 0 0 E 01 1 1 . B00000E 01 2 2 .2 0 0 0 0 0 E 01 2 2 .2 0 0 0 0 0 E 01
T -T fflfr r a i wr r » ---------------------- v -B if t . pot w s — w
O t& tlN C E S TO NESH INTERVAL IN TERFACES
J2
o K T . '6 4 .5 0 3 4 1 1 1 .7 2 3 5 1 2 9 .0 0 6 6 1 4 4 .2 3 3 7 1 5 8 .0 0 0 8 1 6 4 .8 8 5 9 1 7 1 .4 9 3 ,; 0 1 7 7 .8 5 7
I t M 4 .4 0 0 13 i l 4 . 0 d 0
12
O I S T .1 5 .0 0 0 3 3 0 .0 0 0 4 4 8 .0 0 0 5 6 6 .0 0 0 6 7 7 .0 0 0 7 8 8 .0 0 0 8 9 9 .0 0 0 9 1 1 0 .0 0 0
DISTAN CES TO FLUX P O IN TS
J 0 I S 7 .I
10~ w . 6 i r110*954
2 7 9 .0 0 0 11 1 9 1 .9 4 0
a i d i . 9 S 8 12 2 0 4 .9 0 8
4 1 2 0 .6 * 4 S 1 3 6 .8 3 2 6 1 5 1 .2 7 3 7 1 6 1 .4 7 9 8 16 8 .2 2 1 9 1 7 4 .7 0 4
1 O I S T .T 775O T 2 277309 1 S 9 . S W f T 7 . f i I 6 5 717553 6 S 2.SO O f 9 3 .5 0 0 8 1 0 4 .5 0 0
i m INPUT SV RESIGN-------22 22 22 22 22 22---------g I P 1 2 T i 2V n
7 9 11 I S 19 21--------2----- « — 4 14 I V 21
I 3 S 13 I f 21
CONE NUMBER AT EACH NESH INTERVAL
1 2 3 4 5 6 7 0 9 10 11 12
22 22 22 22 22 22 22 22 22 22 22 22 i l 2T ? 2~» 22 I I ' 2 2 ' 22 2 0 2 »
• • 10 10 12 12 1* I * 2 0 20 2 1 211 r n i n n n i » » a 212 2 4 4 * * 14 14 10 1 » 21 212 -2 4 ~ 4 4 4 14 14 1 « t « 21 2 F1 1 3 3 ) 5 13 13 17 17 21 21
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NUCUOE CHAIN DESCRIPTIONS
S1C.SET I THROUGH 2 CONTAIN T CHAINS
oecaV CAPTURE i V IC i f f MufiLfSE i d • • i i 14 IS 16 17
new c h a i n s t a r t s ..........................12 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0 0 .014 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0 0 .045 0 .0 0 .0 0 .0 0 .0 f l.O ....... 0 .0 0 .016 0 .0 O 0 .0 o.4 3 .0 o .c 0 .017 0 .0 0 .0 0 .0 ___o,o _0,0 0 .0 . . 0 .0
NEW CHAIN STARTSlO - 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0l l 0 .0 0 .0 0 .0 0 .0 0 .0 .......0*0 ..... ______ ____________ _____________
HEM CH AIN S TA R TS ............... ................. .............................................................................................. ......................................................563FN CAPT *10000 9000 0 .0 2 7 0 0 0 0 0 .0 3 0 0 0 0 0 0 .0 3 0 0 0 0 0 0 .0 2 7 0 0 0 0 C.03COOOO 0 .0 2 7 0 COO 0 .0 3 0 0 0 0 0
___________ 64________________________0.0 0.0 0.0 0.0________OjO________0 .0 0.0_______57 o .o ib o too o.osooodo 0.0200000 o.oisoooo o.ozooooo o .c i30000 0.0200000
H S tC fflf f f iiT t f T S----------------- ---------------------------------------------------------------------------------------------------------------------- -----------------------------------------------____________ 563FN CAPT OlOOOO 1000 0 .0 2 7 0 0 0 0 0 .Q 300C C0 0 .0 3 0 0 0 0 0 0 .0 2 7 0 0 0 0 0 .0 3 0 0 0 0 0 0 .0 2 7 0 0 0 0 0 .0 3 0 0 0 0 0
65 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0 0 .0267
NEW CHAIN STARTSH 0.0714949 0.0600046 tf.06600bQ~b.O>i4999 0.0600000 0.0714999 0.0603000
NEta CRAIN STARTS ' ' 76 1 .5 0 1 0 9 9 6 1 .5 4 6 5 3 5 4 1 .5 4 6 5 9 9 4 1 .5 0 1 0 9 9 6 1 .5 4 6 5 9 9 4 1 .5 0 1 0 9 9 6 1 .546S 994
NEW CHAIN STARTS77 Q„0*3400:1 0«6i34600 0 .0 1 3 4 0 0 0 0 .0 1 3 4 0 0 0 0 .0 1 3 4 0 0 0 0 . C l 34000 0 .0 1 3 4 0 0 0
C M Ik AteflfSV < ' n 3 0 0
4 T ' & i t 1 2 0 5159000 16 18 0 5151000 17 218 0 14 0 19 0 2 0
FUEL MANAGEMENT IN PU T FOR CASE T I T L E - H U L T I-C V C L E BREEDER (SHEAREO RODS A D JU S TED . RECYCLE FEED DETERM INED>12X6X3 GROUPS*'288 POINTS I R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
OATA P iL E S AND CORRESPONDING I/ O U N IT NUMBER^ FOLLOWMANGDATA-21 SCRATCH1-22 H IS T D A T A -2 3 C Y C LH 1 S T-2 4 M ASSDATA-25 SB IN D EN S-26 ZQNEOENS-27 SCRATCH2-2B F U E 1 0 A TA -2 9
INPUT DATA PROCESSING FOLLOWS_______________________________________________________________________________________________________________
FUELING* MAKEUP* AND DISCHARGE STREAMS IN PUT DATA _ S EC TIO N 091
GENERAL DESCRIPTIO N 5 7 1 0 0 0 1 0NUCLIDES TO BE TREATED 10 11 12 14 15 16 17
OfeCAV OAT A16 0 1 .7 0 0 0 0 E — 09
FEED STREAM DATA*1 0 0 ^ . 0
0 0 0 .0
0 0 0 0 .0
0 0 0 0 .0
0 00 .0 0 .0
2 1 0 0 .0
0 0 0 .0
0 0 0 0 .0
it 0 0 0 . 0
0 00 .0 0 .0
2 .2 9 3 7 6 E— 05 3 1 0
O .B 0 0 0
7 .5 2 6 5 0 c— 03 0 .0 0 0 0 0 0 0 0
0 .0 0 .0 0 .0
0 .02 .3 9 8 2 0 E -0 5
0 .00 .0
0 .0 0 .0 5<.86970E“ 03 0 .0
0 .00 .0
0 .00 .0 0 .0
4" 1 0 0 .0
0 0 0 .0
0 IT 0 0 .0
0 0 00 . 0
0 00 .0 0 .0
2 .31200E - 05 5 1 0
0 .0 0 0 0
7 .5 8 6 8 0 E -0 3 0 .0 0 0 0 0 0 0 0
0 .0 0 .0 0 .0
0 . 0 4 .3 1 8 3 0 E -0 5
0 .00 .0
0 . 0 0 .0 1 .4 1 7 0 0 E -0 2 0 .0
0 .00.0
0 .00.0
rovnvn
o .o
MAKEUP STREAM DATA1 0
0 .01 0 0
0 .02 0 0
0 .02 .8 6 9 6 0 E -0 1 0 .0
l.O O OO O E 00 l.OOOOOE0 .0
r*o i.o o o o o e9 .9 6 0 0 0 E— 01
00 l.QOOOOE 002 0
0 .01 0 0
0*03 0 0
0 .03 .2 8 1 7 0 E -8 1 0 .0
l.O O OO O E 00 l.OOOOOE0 .0
00 l.OOOOOE9 .9 6 0 0 0 E— 01
00 l.O O OO O E 00-■ J 5
0 .01 0 0
0 .04 0 0
0 .03 .8 4 8 7 0 E -0 1 0 .0
l.OOOOOE 00 l.O O OO O E0*0
00 l.OOOOOE9 .9 6 0 0 0 E -0 1
00 i .o o o o o e oo♦ 0 0 0 0 «A 0 0 l.OOOOOE 00 0 .0 0 .0 9 .9 6 0 0 0 E -G 1
l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.O O OO O E 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 005 - 0 0 0 — ft 1 O ' 0 i.o o O o o e 00 0 .6 0 .0 9 .9 6 0 0 0 E -0 1
l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.O O OO O E 00 l.OOOOOE 00 l.OOOOOE 00 l.O O OO O E 006 0 0 0 0 1 0 0 l.O U U U U t 0U 0 .0 0 .0 9 .9 6 0 0 0 E -0 1
l.OOOGQE 00 l.OOOOOE 00 l.OOOOOE 00 l.O O OO O E CO l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 007 0 0 0 0 1 0 • 0 l.OOOOOE 00 0 .0 0 .0 9 .9 6 0 0 0 E — 01
l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00
DISCHARGE STREAM DATAI 5 BH 5 5 0 5 5 575 2 . 06600E 02 STo 9 .9 5 0 0 8 E -0 1
l.OOOOOE 00 l.OOOOOE 00__ l.OOOOOE 00 l.O O OO O E 00 l.OOOOOE 00 l.OOOOOE 00 l.OOOOOE 00
FUEL MANAGEMENT DATA - SEC TIO N 093
CARD 2
1 O O 6 — J5 0 & 4 4 C 0 Q t 0 5 5 l O O O O U Q O
CAROS 3 AND * 0 .0 0 .0 0 .0 0 . 0 2 .5 0 0 0 0 E —03 0 .0Ood 1 .0 0 0 0 0 E -0 2 l.O P O O O E -0 2 l.OOOOOE 00 l.OOOOOE 00 0 .0
C U K 4*
CMOS 5« OR DEFAULTI.oooooe 00 i.oooooe oo i.oooooe oo i.oooooe oo l.oooooe oo i.oooooe i.qujcoe qo l.oaooot u<i i.oq-- mi.oooott 00 I.OOOOOE 00 i.oooooe 00
1 1 i 1 0 0 0 1 0 0 1 1 0 0 02 I I 2 4 A 6 1 6 0
... r2 0 0 0
3 1 3 3 0 0 0 1 0 0 1 3 0 0 04 1 4 4 6 0 0 1 0 0 1 4 0 0 09 1 S 9 0 0 0 1 0 0 1 5 0 0 06 i 6 6 0 0 0 1 0 0 1 6 0 0 07 i 7 7 0 0 0 1 0 0 1 0 16 20 0 15 19 0 14 lf l 0 13 I T 0 0 a
f ISJiftt nuCl 1TOS--“ f iT T T 16--------------------------------------------------------------------------F E R T IL E NUCLIOES------- 12 ISI nT R ^ S U tE MUtllOlS----NOtoE SP?CJPI66OTHER NUCLIOES------- l l 17SWUCTUKIL HDCL1PE5— i r » ~ i y TI --------------------------------------------------------------------------------SP ECIA L N UC LIO ES— 25FUSION IHflODCT" HuCLTGfl-— ~W~ S5T U 6 i t i f t -------------------- --------------
COKF STQRICF BWT E W WCE I UWPS T t OUAT ! Oln CPXSTA M 5 I7P T M TEA5 Tf f " y ia « f >-----------iS V
EWTCTOn M «T B «T I_iiTLL_BT STbtiEb I n tAM----------------------------------------------------------------------------------------------------------------------------------------------
HUriftEft W — -C O L M R 5 . '5 0 « i . M .A S E S , « 0 u « 7 ~ u * S C i T , B O N N S iU f, ftffiio N S . a n P ZONES----------------12------- S------- i --------i ------- o------- 2 ~30H I j
HWOKT CO«T tOMS M5EHVE0 P0H~P1 U 5lfWACE=— 40000------------------------------------------------------------------------------------------------------------------MEMORY LOCATIO N S USEO FOR T H IS PROBLEM----------------- 12028HEHOiV LOCATIONS WOT U$£g=--— -------- 17TH ------------------------------------------------------------------------------------------------------------------------------
A iL U k - EIGENVALUE PROBLEM #OLLOWS #OR CYCLE 1 CYCLE TIM E 575 OAVS TOTAL TIM E 57o DAYS
M U LTI-C Y C LE BREEDER ISMEARED ROOS A O JUSTEP t RECYCLE Ft;ED OETERM INEOI________________________________________________12X6X3 GROUPS. 2W8 PO IN TS I R - 2 ) . STREAM OF C IT A T IO N CASES ORNL 72
L IN E RELAXATION M ILL BE PONE ON ROWS ANO COLUMNS - 1 INNER I T E R A T I O N S ! ________________________________________________________________L IM IT IN G VALUES OF THE SEARCH FACTOR FOR ABSORPTICM ANO TO TA L LOSS ARE -2 .3 7 8 2 7 E OO -4 .8 2 6 0 2 E OOIT E R A TIO N FLUX CHANCE BETA MU-1________ M U-2 M U-3________________ K SEARCH FACTOR____________________________________________
CROSS SECTIONS UPDATED W ITH 6 .9 9 8 2 2 0 -0 2_________________________ ___________________________________________________________________ CROSS SECTIONS UPDATED W ITH -2 .2 8 & 4 B O -Q 3 ______________________
25 2 .6 4 1 6 8 E -0 4 T T S S I T i 2 7 7 l ' » ? 1 .1 4 9 4 5 2 .0 8 5 7 3 1 .0 0 0 0 1 8 8 .2 5 4 0 6 0 -0 5
CONVERGENCE IN D IC A TIO N BY M IN (H it IN C THE SUM O f tH E SQUARES OF THE R E S I0 0 ES - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 6 7 K 1 .0000172
END OP C M T 1CA L1 T V SEARCH - ITER A T I ON T ltfE ' ft.fo’T H lB u f B ---------------------------------------------------------------------------------------------------------------------------------------------------------------
INPUT R E L A TIV E CONCENTRAtION CHANGE TIMES 6 .7 6 9 S 6 E -0 2 HAS B E E N T o DED TO TH E I N I T I A L SEARCH CONCENTRATIONS
T k A C fk d N ABs URP?«On IN SEARCH NUCLTo H 0 .0 1 5 0 7 8
LEAKA6S 1 .41160? |8 Tb TA L LOSSES 1 .1 2 0 0 0 E 20 TO tA L PRODUCTIONS 1 .1 2 0 0 0 E 20 REACTOR POWER!MATTS! 2 .5 7 7 3 2 E 09
K U L Ti"C Y C L E BREEDER ISMEARED RODS AD JU S TEO . RECYCLE FEED DETERM INED)12X8X3 CROUPS* 288 P G IN TS ( R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
Nu m m a r y OF NEUTRON LO S SES, E T C . BEFORE D EP LETIN G STEP 1 OF CYCLE 1 TO TAL D EPLETION T IN E 0 .0 OAYS
ZONE CLASS CORE A l
F IS S IL E0 .1 1 9 8 0
F E R TIL E0 .1 5 3 7 3
INTERM EDIATE0 .0
OTHER STRUCTURAL 0 .0 0 0 8 7 0 .0 1 3 9 3
SPECIAL0 .0 0 0 2 5
UN S P EC IFIED0 .0 0 6 7 2
SUNS0 .2 9 5 2 9
CONV. R A TIO 1 .1 0 1 3 0
POHERIMW) 8 .7 3 9 6 6 E 02
F IS S IL E IK G I 8 . 71813E 02
CORE A2 CORE A3
0 .1 2 8 3 50 .0 9 5 9 2
0 .1 5 2 2 10 .0 9 8 1 3
0 .00 .0
0 .0 0 0 9 40 .0 0 0 7 2
0 .0 1 3 3 60 .0 0 8 6 0
0 .0 0 0 2 30 .0 0 0 1 5
0 .0 0 6 2 90 .0 0 4 0 1
0 .3 0 1 3 90 .2 0 7 5 3
1.0 0 2 100 .9 4 9 3 5
9 .4 2 8 7 8 E6 .9 9 8 6 5 E
0292
9 .9 3 2 7 6 E 02 1.1 5 7 9 4 E 03
61NK £1 BLNK C2
0 .0 0 1 0 40 .0 0 0 9 6
0 .0 * 9 * 30 .0 3 6 2 7
0 .00 .0
0 .00 .0
0 .0 0 3 3 70 .0 0 3 0 1
0 .0 0 0 1 30.0 0010
0 .0 0 0 0 40 .0 0 0 0 4
0 .0 4 3 9 00 .0 4 0 3 8
3 6 .6 7 0 0 93 6 .6 0 8 2 2
1 .4 0 8 2 0 E1 .3 5 9 6 3 E
0101
2 .0 8 5 4 7 E2 .2 1 0 0 8 E
0101
8 INK CJ BLNK B l
0 .0 0 0 6 00 .0 0 110
0 .0 2 2 7 30 .0 4 1 9 1
0 .00 .0
0 .00 .0
0 .0 0 1 8 70 .0 0 2 3 6
0 .0 C 0 0 60 .0 0 0 0 4
0 .0 0 0 0 30 .0 0 0 0 6
0 .0 2 5 2 90 .0 4 5 4 8
3 6 .5 8 1 2 83 6 .3 1 1 3 1
8 . 76461E 1 .9 3 9 3 0 E
0001
2 .2 4 3 1 9 E 01 3 .7 6 5 6 4 E 01
SINK B2 RFLTR E
0.0 0 0 4 80 .0
0 .0 1 8 1 00.0
0 .00 .0
0 .00 .0
0 .0 0 1 0 50 .0 0 3 0 1
0.000020 .0 0 0 0 4
0.000010 .0
0 .0 1 9 6 50 .0 0 3 0 5
3 6 .9 3 5 5 50 .0
4 .8 1 2 9 3 E0 .0
00 3 .7 6 5 6 6 E0 . 0
01
h F itrt 6 0 .6 6 .4 0 .6OTHER LOSSES
0 .0 0 .0 0 5 3 4 0 .0 0 0 0 7 0 .0 • BASED ON S T A R T -C F -S T E P TO TAL LOSSES
0 .0 0 5 4 20 .0 1 2 6 2
0 .0 0 .0 0 .0
OVERALL 0 .3 4 8 2 6 0 .5 6 2 4 0 0 .0 0 .0 0 2 5 3 0 .0 5 5 8 9 0 .0 0 110 0 .0 1 7 2 0 1.0000 0 1 .4 2 1 9 7 2 .5 7 7 3 6 E 93 3 . 16373E 03
POWER NORMALIZATION 0 .9 9 5 1 7 * MAXIMUM POWER D E N S ITY 4 .8 0 5 2 9 5 E 02 IN ZONE 3 AT END SUBSTEP 1
AFTER STEP 1 OF CYCLE I t THE TIM E IS 7 5 .0 0 0 0 OAYS. THE TIM E STEP HAS 7 5 .0 0 0 0 DAY S . AND TO TAL TIM E IS 7S.OQOO OAYS ft**********************-**. «**••**•**•**••»**•••»*»•**•***•••*••*•**♦**♦**•**?••*•**#••*****•******•••#**•«***•*•**•*•**••#£ ro
V I0 0
M U L TI-C Y C L E BREEDER (SHEARED RODS A C IU S TE O . RECYCLE FEED DETERM INED!12X8X3 GROUPSr 288 P O IN TS ( * - 2 > . STREAM OF C IT A T IO N CASPS ORNL 72
SOnMAry OF MEuTftdN L ffS S fS , f t c . f o r s te p i c y c le i a t c y c l e d e p le t io n t in e 3 7 .5 0 d a y s , f i s s i l e k g i s a t 7 5 .0 0 oays
ZONE CLASS F IS S IL E F E R TIL E IN TERM ED IATE OTHER STRUCTURAL SPECIAL U A S P EC IF IEO SUNS CONV. R A T IO P Q H E M M I F I S S l L C t K G iCORE A I __________ 0 .1 2 0 1 2 0 .1 5 3 0 0 0 . 0__________ 0 .0 0 0 8 9 0 .0 1 3 9 3 0 .0 0 0 2 5 0 .0 0 7 3 8 0 .2 9 5 SB 1 .0 9 2 6 3 8 . I S 562E 02 8 .7 T S 9 7 E 02CORE A2 CORE A3BDJiTCrBLNK * C2s o s rs rBLNK B1ST.Sk Si~ RFLTR Ei F c m r
0 .1 2 8 2 30 .0 9 5 5 10.06155"0 .0 0 1 3 7
0 .1 5 1 5 40 .0 9 7 8 7a . r a m0 .0 3 6 2 1
"575H TT0 .0 4 1 8 6
1 ) . 01809 0. 0 '
TJ75-----------
0.00.0
0 .0 0 0 9 60 .0 0 0 7 2
0 .0 1 3 3 60 .0 0 8 6 0
0 .0 0 0 2 30 .0 0 0 1 50 .0 0 0 1 30.00010
0 .0 0 6 9 50 .0 0 4 3 2
0 .3 0 1 2 70 .2 0 7 1 6
0 .9 9 8 2 3JblSte2-
9 .4 1 8 0 5 6 02 6 .9 7 2 6 3 E 02
9 .9 2 4 3 2 E 02 I .1 4 8 8 7 E OS
" 5 ^ r0.06 .00.00 .60.0
■578"
0 .0 0 0 0 00 .0 0 0 0 0
0 . 0 6337"0 .0 0 3 0 1
0 .0 0 0 0 50 .0 0 0 0 5
0 .0 4 4 3 40 .0 4 0 7 4
2 4 .6 1 5 3 12 5 .5 2 3 9 0
1 .6 8 3 4 3 E 01 1 .5 8 5 2 S E 01
4 .1 9 2 2 5 E 01J U l S I S f l f c J U
0 .0 0 0 7 5 "0 .0 0 1 4 8o .o o o S s9 .0
T57TJ------
0.000000.000000.00000o .o
7 7 5 ------------
0 .0 0 1 8 70 .0 0 2 3 60 .0 0 * 0 50 .0 0 3 0 10 .0 0 5 3 4
0 .0 0 0 0 6C .0 0 0 0 4
0 .0 0 0 0 30 .0 0 0 0 7
0 .0 2 5 4 30 .0 4 5 8 0
2 8 .7 6 9 8 22 7 .1 3 8 1 8
0.000020 .0 0 0 0 46 .6 0 0 5 V
0 .0 0 0 0 10 .0
0 .0 1 9 7 10 .0 0 3 0 5
3 2 .2 9 7 6 70 .0
9 .6 4 9 3 5 E 00 2 .I4 3 8 5 E 015 .1 8 2 4 8 E
S l S .00
3 . 46470E 01 A J I B i L 0 14 .7 5 8 9 2 E 010 .0
0 .0OTHER LOSSES* 8ASE0 ON S T A R T -O F -S T E P TOTAL LOSSES
0 .0 0 5 4 2A f l l l t f .
0 .0 0 .0 0 .0
OVERALL 0 .3 4 9 5 7 C . 56052 0 .0 0 .0 0 2 5 7 0 .0 5 5 8 9 0 .0 0 1 1 0 0 .0 1 8 8 6 1 .0 0 0 0 0 1 .4 1 1 5 7 2 .5 8 3 5 9 E 03 3 .2 4 4 4 6 E 03
TIM E STEP THERMAL ENERGY* MM-HRS 4 .6 S 0 4 6 E 0 6 AND TOTAL IS 4 .6 5 0 4 6 E 06
TIM E STEP 1 REQUIRED 0 .0 7 S M INUTES CPU T IM E , AfcP 0 .6 3 6 M INUTES CLOCK TIM E
A FLUX * EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 1 C Y C IE TIM E 7 5 .0 0 0 0 OAVS TOTAL TIM E 7 5 .0 0 0 0 OAYS
IV E ftA V IM F l u x CHANCE----------BFT7T H O = T n o = r N U -3
18 4 .2 9 1 5 3 E -0 5 ____1 .3 9 1 7 4 -0 .6 6 9 7 2 -0 .6 6 2 5 2 1 .0 5 8 8 9
K SEARCH FACTOR CROSS SEC TIO N S UPDATED K IT H 7 .9 1 5 2 4 0 -0 3 CROSS SECTIONS UPDATED N IT H -2 .7 4 5 8 6 0 -0 4
1 .0 0 0 0 0 3 1 .5 6 8 7 5 0 -0 5 _______________________
CONVERGENCE IN D IC A TIO N BY M IN IN IZ IN G THE SUM OF TH E SQUARES O f THE RESIDUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 1 0 K 1 .0 0 0 0 0 3 8
ENO O F C R IT IC A L 1 T Y SEARCH - IT E R A TIO N T IN E 0 .0 4 2 MINUTES
IN P U f R E LA TIV E CONCENTRATION CHANGE TIM ES 7 .M 0 6 5 E -0 3 HAS EEEN AOPicO TO THE IN I T I A L SEARCH CONCENTRATIONS
FR ACTIO N ABSORPTION IN SEARCH N UCLIDES 0 .0 1 6 6 7 3 ______ _________________________________________________
LEAKAGE 1.44623E 18 TOTAL LOSSES I .1 2 0 2 5 E 20 TO TA L PRODUCTIONS 1 .1 2 0 2 5 E 20 REACTOR POWER!MATTSI 2o57732E 0 9
rov nVO
PtWW NDRNXL1ZATKW----- WHIHOH WBHTKWSMV 4 .TIW 3IE 6 M h -----------------------3 AT £h5' SubST& ------ T
AFTER STEP 2 OF CYCLE 1* IH F T IN E I S 1 5 0 .0 0 0 0 OAYS. THE T|M E STEP MAS 7 5 .0 0 0 0 O AYS. AND TO TA L TIM E IS 1 5 0 .0 0 0 0 OAYS
M U LTI-C Y C LE BREEOER ISNEAREO ROOS AD JUS TED , RECYCLE FEED O ETER H IN EO I12X8X1 GROUPS, 288 P O IN TS < R ~ 2 ». STREAM OF C IT A T IO N CASES ORNL 72
SUMMARY OF NEUTRON LO S SES. E T C . FOR STEP 2 CYCLE 1 AT C y Cl E D EP LETIO N T IN E 112*90 O AVS. F I S S I i r , K6 I S AT 150*00 DAYS
ZONE CLASS CORE A l
F IS S IL E0 .1 2 2 9 6
F E R TIL E0 .1 5 3 8 7
INTERM EDIATE OTHER STRUCTURAL SPECIAL 0 .0 0 .0 0 0 9 3 0 .0 1 4 1 3 0 .0 0 0 2 6
U N S P EC IFIED0 .0 0 9 9 3
SIMS0 .1 0 1 2 8
CONV* R A TIO 1 .0 7 4 4 0
P O N E R IW ) 0 .9 1 8 9 9 E 02
F IS S IL E IK G I 8 . 82248E- 42
COR6 A2 CORE A3
0.1& 6110 .0 9 2 2 8
£* 14806 0 .0 9 4 8 4
0 .00 .0
0 .0 0 0 9 70 .0 0 0 7 2
0 .0 1 3 1 60 .0 0 8 3 8
0*000230 .0 0 0 1 5
0 .0 0 8 7 >0 .0 0 9 1 8
0 .2 9 7 2 80 .2 0 1 9 4
0*990160 .8 9 2 6 6
9 .2 6 9 3 8 E 02 6 .I4 4 1 8 E 02
9 .9 1 0 2 BE 02 I . K 0 2 2 E 0 3
SIR* Cl ....BLN* C2
5.002690 .0 0 2 2 0
" O i f l M "0 .0 3 6 3 3
0 .00 .0
0.600000 .0 0 0 0 0
0 .0 0 3 4 80 .0 0 3 0 3
o.ooois0 .0 0 0 1 0
0 .0 0 0 0 70 .0 0 0 0 7
0.04681T0 .0 4 L 7 3
14*8129319*94196
2 .S 8 7 4 9 E 01 2 .0 9 7 8 0 E 01
6 .3 0 1 8 4 E 01 6 .0 4 8 7 9 E 01
BLNK C3 BLNK 81
0 .0 0 1 0 70 .0 0 2 1 6
0 . 02248 0 .0 4 1 0 5
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 0
0 .0 0 1 8 60 .0 0 2 3 2
0*000060 .0 0 0 0 4
0 .0 0 0 0 40 .0 0 0 0 9
0 .0 2 9 9 10 .0 4 9 6 6
2 0 .2 2 7 3 9 1 «* 11472
1 .1 4 9 8 S E 01 Z . M l t t f 01
4 .6 5 4 7 5 E 01 8 .1 2 4 3 8 E 0 1
BLNK 82 RFLTR E 0 ,0
o .O if S r0 .0
0 .00 .0
6 .0 0 0 0 00 .0
0 .0 0 1 0 40 .0 0 3 0 0
C *90002 0 .0 0 0 0 4
0*000010 .0
0*019660*00304
29*84329 0*0 ..
6 .0 4 5 1 1 E 00 0 .0
9* 73394E 01 0 .0
6.0 5*0 0 .0 0 .0 0 .0 0 9 9 0 C.-6SSS7 0 .0 0 0 0 0 OTHER LOSSES* BASED ON S T A R T -O F -S T k P TOTAL LOSSES
0*009570 .0 1 1 8 6
0 .0 0 .0 0*0
OVERALL 0 .3 4 9 7 1 0 .9 9 5 0 8 0 .0 0 .0 0 2 6 3 0 .0 9 9 8 8 0 .0 0 1 1 0 0 .0 2 3 7 3 1 .0 0 0 0 0 1 .3 0 5 7 7 3 .3 2 2 1 2 E 0 3
TIM E STEP THERMAL ENERGY. MM-HRS 4 .6 4 9 9 6 E Oft AND TOTAL IS 9 .3 0 0 0 2 E 06
TIM E STEP 2 REQUIREO 0 ,0 6 9 M INUTES CPU T IM E . AAO 0 .6 3 8 HIW UTES CLOCK TIM E
A F IN A L FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 1 TO TA L D EP LETIO N T IN E 190.000 DAYSI TERAT ION FLlix C'tMCE-------- ifTK -----------T R F I-------------JSFZ------------ iu=5-------------------------K---------- S H S e iT R C fS i-----------------------------------
CROSS SECTIO N S UPPATEO N lT H 6 .9 9 2 2 3 0 -0 3 CROSS SECTIONS UPOAtEO M1TH -2 .3 7 2 8 0 0 -0 4
IB 3 .4 3 3 2 3 E -0 5 1 .3 9 1 7 4 -0 .6 2 4 6 9 -0 .6 6 8 4 9 t .0 9 0 7 0 1 .0 0 0 0 0 3 1 .4 4 0 3 1 0 -0 9 Mo \
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G T H i SUN OF THE SQUARES OF TH E RESIDUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 1 0 it 1 .0 0 0 0 0 3 8 O
ENO OF C R 1 7 IC A L ITY SEARCH - IT E R A T IO N T f»lE 0 .0 3 9 PIN U fES _______________________________________________________________________________________________
INPUT R E LA TIV E CONCENTRATION CHANGE TIM ES 6 .3 5 4 9 4 6 -0 3 HAS BEEN ACOEC TO THE I N IT I A L SEARCH CONCENTRATIONS
FRACTIO N ABSORPTION IN SEARCH NUCLIDES 0 .0 1 7 9 6 7 _________________________________________________________________________________
LEAKAGE 1.48245E 18 TOTAL LOSSES 1 .1 2 0 4 9 E 2 0 TO TA L PRODUCTIONS 1 .1 2 0 4 9 E 20 REACTOR PO hER lM ATTSl 2 .5 7 7 3 2 E 0 9
M U LTI-C Y C LE BREEDER (SHEARED ROCS A D JU S TED . RECYCLE PEED DETER H IKED )12X8X3 CROUPS, 288 P O IN TS I R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
F IN A L SUMMARY OF NEUTRON LOSSES* ETC • FOR CYCLE 1 TO TA L D EP LETIO N TIM E 1 5 0 .0 0 DAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 * 4 1
F E R TIL E0 .1 5 5 1 0
IN TERM ED IATE OTHER STRUCTURAL 0 .0 0 .0 0 0 9 6 0 .0 1 4 3 0
S P ECIA L0 .0 0 0 2 6
U N S P EC IFIED0 .0 1 0 9 2
SIMS0 .3 0 5 9 4
CONV. R A TIO 1 .0 6 5 0 3
POWER!MW) 9 .0 8 5 9 4 E ~
F IS S I L E (K C ) (1 .8224BE 02
CORE A2 CORE A3
0 .1 2 4 2 40 .0 6 9 7 4
0 .1 4 5 4 1 0 .£ 9 2 3 6
0 .00 .0
0 .0 0 0 9 70 .0 0 0 7 1
0 .0 1 2 9 80 .0 0 8 1 8
0 .0 0 0 2 30 .0 0 0 1 4
0 .0 0 9 7 50 .0 0 5 6 5
0 .2 9 3 5 819678
0 .9 8 6 0 60 .8 5 3 8 1
S a13951E 6 .5 6 1 5 4 E
0202
9 .9 1 0 2 8 E 02 1 .1 4 0 2 2 E 03
BLNK C l BLNK C2
T . b i S S "0 .0 0 2 6 2
o . o i i a s0 .0 3 6 5 3
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 0
0 .0 0 3 6 00 .0 0 3 0 4
0 .0 0 0 1 40 .0 0 0 1 0
0 .0 0 0 0 90 .0 0 0 0 8
0 .0 4 8 9 50 .0 4 2 3 8
1 2 .3 3 6 0 61 3 .4 3 6 8 5
2 .8 3 0 8 3 E 01 2 .3 8 8 3 8 E 01
6 .3 0 1 8 4 E 01 6 .0 4 8 7 5 E 01
BLNK C3 BLNK B l
0 .0 0 1 2 20 .0 0 2 4 7
0* 62233 0 .0 4 0 4 0
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 0
0 .0 0 1 8 40 .0 0 2 2 8
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 40 .0 0 0 0 9
0 .0 2 5 4 90 .0 4 5 2 9
1 7 .6 4 0 0 81 5 .5 9 5 6 6
1 .2 4 6 4 3 E 01 2 .I3 5 9 2 E 01
4 . o5475fc 01 8 .1 2 4 3 8 E 01
BLNK B2 RFLTR E
0 .0 0 0 7 40 .0
0 .0 1 7 7 80 .0
0 .00 .0
0 .0 0 0 0 00 .0
0 .0 0 1 0 30 .0 0 2 9 9
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 20 .0
0 .0 1 9 5 80 .0 0 3 0 4
2 3 .5 0 5 9 10 .0
6 .5 3 3 9 4 E 0 .0
00 5 .7 3 3 5 4 E 01 0 .0
■ r f t u t s ... 0 .0 O .tf” O .Uo t h e r
0 .0 0 .0 0 5 6 5 0 .0 0 0 0 8 0 .0 LOSSES* BASED ON S T A R T -O F -S T E P TO TAL L O S S -S
0 .0 0 5 7 30 .0 1 3 2 4
0 .0 0 .0 0 .0
OVERALL 0 .3 4 8 7 2 0 .5 5 1 7 0 .0 0 .0 0 2 6 5 0 .0 5 5 8 9 0 .0 0 1 1 1 0 .0 2 6 6 4 1 .0 0 0 0 0 1 .S 9 0 2 7 2 .5 7 7 3 3 E 0? 3 .3 2 2 1 2E 03
M U LTI-C Y C LE BREEDER ISMEAREP ROCS A D JU S TED , RECYCLE FEED DETERM INED!~ ~ 12X8X3 GROUPS• 288 P O IN TS f R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
5TAftr T UEC TWMACEWEN r PAR TVCLE-----1------------ ----------------------------------------------------------------------------------------
a r r a y St o r a g e a l l o c a t e d f o r f u e l m a n a g e m e n t i s <*o c c oT H !S FUEL MANAGEMENT PROBLEM REQUIRES *796________________________________________________________________________
END FUEL MANAGEMENT FOR CYCLE 1_______________________________________________________________________________________
CYCLE 1 REQUIRED 0 ,2 7 * MINUTES CPU T IM E , AND 3 .2 7 9 M INUTES CLOCK TIM E
M U LTI-C Y C LE M E E 0 6 R 3SMEARE0 RODS A O JU S TEO . RECYCLE *££C O frE JM fN E O t!«»*> GMmv m w m i r u - « .-------s rtt'f lrw ch a tto * tm rtsnia ---------------------------------------- -—
~k ? m r - T nC HIW EW W BSCEW P fc lM r r f lT r t M I " t t f C T TTH f---------- t t -------- 55y5— i m T T m — iso.oooo OAYS-
L IN E RELAXATION II1LL BE POKE ON ROWS AM ) COLUMNS - 1 »W .g > IT E H A TI0 N 1 S )_______________ ______________________________________________________L i l i l f i k e VALUES OF t h e s e a r c h f a c ^ 1* FOR a b s o r p t i o n ANO TO TA L LOSS ARE -2 .4 4 7 0 0 E 00 -4 * « M 9 V e 0 0 I I C M A T im FLUX CHANGE BETA N t f - l N U -2 M U -3 K SEARCH FACTOR
------------------- --------------------------------------------------------------------------------------------------------------------------------------------------------a 6 i r i | i E ¥ u f o a t e d w i t h i . m i i o ^ o i ----------------------------------------4. ^ ™ c*°*s SECT lows UFOATCO with a a « s » ____,___ _ _____n 6 .t * l t i9 E -0 5 1 .5 * 1 7 * • t . U S S - T T l 19551 1731713 t *000006 2 .7 9 7 « 0 0 -0 *
CONVEUCNCe 1 WfflC AT fWTIV MM(HI2Il46 THI SuM «5f VMc SQUARES OF ¥h£ *fcsi0urs - R E L A TIV E ABSOAP H O N 1 .0 0 S 3 0 1 9 K 1 .0 0 0 0 0 5 7
twrnr egiTicAirrv "aaror"iir e n i ring o.a%o Mwm------------------------------------- --------------------------------------~i w pUT~ iF .r A T T ^ t caKcewtM Ai iOH c t i t t s r t t H K — r i f s u t - ^ t m m i o t o m i N i T u r u A R c * c o w e n t k a i io n s
’ F f f ic r ia N ~ X B s a M ? iw ~ !M s s w e a s u t n u n — n . s i r m ---------------------------------------------------------------------------------------------------------------------------------------------------- ‘
T E IK W E v m i n f T OT AL I S S U i r . n W g T f f " W n i . ' M f l 6 i t t t M M k . l a t t w - i b " K A t t o R P o k M ^ V i s ) " 2 .> ? 7 3 2 E ~o s
WLH-CVCLE BREEOER ISNEAfi£0 RODS ACJl'iTEO. RKCVUC PCiO OCIMM1MOI- i i x t f k r i i i b l F S , 2» » * » o i* U *R-i»7---Wukn » aUirnt cases mmTW
-wwai ? op ktuifcflN lo»«s, m . *g«*t w a i i u r sw i » t * t a
" T B R i n E C S f r " CORE M
■ c w n r e --------------CORE 43- f f t S i T T j --------------
»INK C2SIN K C3 8LNK B1 81WK *2
r f s s r c i r0 .1 2 3 2 1
" K T J f n r0 .0 1 1 2 6<>•662*40.00220
6 .1 5 4 7 2 0 . 0 0 .c a 0 » 3 0 .0 1 4 2 0 0 ,0 0 0 3 * 0 « 0 0 » » 3 _____________"57FE75S 5 T o : ! b . & c o « 0 . 0 130 ? o . e o o » o . o e i no . o < » m o .o
“3 W »T jyeus.
COMV. R A IIOusmsh
T T H 5 V W0 .0 3 S 4 *
TPTo . c
0 ,0 0 1 0 70 .0 0 2 1 4
0 .0 2 2 4 30.0 * 0 0 3T O T 0.0_____
13 O.ttOOOt 0.60000 P.PQI03...OiOOOlO .....0.88081
0 .0 4 7 6 S
o«*noo»- M a n .UJlUI
r m i t f i t t ii d a i z i u t
0.0 0.00000 0.00185 O.OOfrOt O.OOOOfc 9.02M ) I0 .2 K U-0*0— -0,00000 0.00230 O.OtMC*__________ fttfigftM__ M S i l f c - I M I M i -
l * 2 d » H I 02 6 2i . H U W O l
2.M21IC 01 k i l l l f f 01
4.0S13M 617 .f ll4 » f lg o i
t . l » S 6 2 f 01 *.§4fc»« Oi
RFLTR■WCTT
'o ' .o o o i i o.o
0.0S.0t e t
0 .0 6 T 3 0
■fef-9.00104 0.00002 0*00002 O .O if i t 2 1 .1 2 2 9 7
_JUSL7. 04?0#l 00
. 1 4 .4.1312M 01 0»C
TS75T W ooOTMga to s s e s * b a se o o h s u r t - o f - s i i * i o u i t o u t s
0.60»*»- g x P i A i l -
0 .0 0.0 0.6
OVERALL 0 .S 4 S 6 3 0 .S S * 3 6 0 .0 0 .0 0 2 4 2 O .O t S W O .-iO H O ____6 _ 1 .0 0 6 0 0 - Bit «? * ran
pdtiik vfetfdiiFffTBN row* OENiiUv «.*?30*2C 02 in im t J w i w iw s r ir 1 !
j r M E j r j i » i g . , « y * * * .....j a s f l m j a a ^ s a J g f H ____m d m j u n .
M U L TI-C Y C L E BAEEfaER <SHEABfcO HODS A D JU S TED . r e c y c l e FECP 0 E 7 E R m »£ 0 >12X0X3 CR ^'JPS, 288 P O IN TS I R - i » . STREAM Of C ifA T 1 0 M CASES 0RNL I ?
T O B C T H y 6F nlEUTfcfr C 3 » » . n i r m m t > T E t Z l T 2 Jit 6 y c le ~ 3 ^ > L e tio 5 ~ ?T HE— 3 n M 0 i 7 s 7 " f i s s i i J ^ u ; t ' T k i — W M ' b i t s
ZONE CLASS CORE A1 CORE A2 CORE A3■roarer —BLNK C2BLW Ci---------BLNK 61
■ T O H T B ? ------------RFLTR ZRFLTA T5---------
F IS S IL E0 .1 2 3 * 30 .1 2 5 0 60 .0 9 0 8 9
"S V W l g " 0 .0 0 2 6 0 6.6 d l i r0 .0 0 2 4 8'5.566460 .0
"575--------
F E R TIL E IN TER M ED IATE CTNER STRUCTURAL SP ECIA L U K S P E C ltlE D SUNS CONV. RAT40_ 0 a 5 3 9 8 ____0*0___________ 0 .0 0 0 9 5 .0 .0 1 6 2 0 C . 00026 0 .0 1 0 5 1 0 .3 0 3 3 3 _______L.0& 6420 .1 4 6 6 2 0 .0 9 3 5 5 6*06111 0 .0 3 6 3 9"5755W0 .0 4 0 7 6
■ f l r o m r0 .0
“575
0 .00.0
t e i to .o
'6 .60.0
0 .0 0 0 9 80 .0 0 0 7 10 .0 0 0 d T o.oocoo O.OOOPO 0.00000
0 .0 1 3 0 ?0 .0 0 60 .0 0 3 0 .0 0 3 0 3
0*0002)0 .0 0 0 1 42 8 0 .0 0 0 1
l a ' o .o o oi0 .0 6 6 i x o .o o o ia
0 .0 0 9 5 1 0 .2 9 5 2 7J f t t i S j U L
0 .0 4 8 0 9A O J g f l L
0 .9 8 6 6 8
P&hERIMf) 9 «Q 0 > 7 > £ 029 .1 9 5 8 7 E 02 6 .6 4 6 1 S E 02
J a U » ^ J 2 9 . 89952E 02 A « I3 » 1 7 E 81
0 .0 0 0 0 90 .0 0 0 0 8
1 2 .3 5 4 9 1.U b t A t t K L
2 .7 5 0 04E 02 2 .3 4 » 2 8 £ a i
7 .3 5 4 1 2 E 01 J b l f t & U C - O l
3 .2 2 8 4 0 E 01 J i i J S I I L I i
" 5 ^ To .u
"575"0 .0 0 0 0 0 0 . 0 o .O
0 .0 0 1 8 50 .0 0 2 3 06 .9 0 1 0 40 .0 0 3 0 2
T O 5 5 5 T
0*000060 .0 0 0 0 40*000020 .0 0 0 0 40*00006
0*00004 0 ^00010
0*02558 17*70657 1 .2 J 8 8 6 C 01
0*00002a .o ____
0 .0 1 9 8 7J M
19*56543J L l f i .
7.39A40EJLSL
00 7 .2 9 1 1 8 E 01JLuSL
0.00000OTHER LOSSES* BASEO ON S TA R T-O F— STEP TO TA L LOSSES
0*005650*01213
0 .0 0 .0 0*0
OVERALL 0 .3 4 9 8 1 0 .5 5 2 5 3 0 .0
T IN E STEP THERMAL ENERGY* MW-HRS
0 .0 0 2 6 5 0 .0 5 5 9 0 0 .0 0 1 1 0 0 .0 2 S B 7 1 .0 0 0 0 0 1 .3 8 8 2* 2 .5 8 2 6 T E 03 1
4 .6 4 9 1 6 E 0 6 A W TOTAL IS 1 .3 9 4 9 2 E 07
TIM E STEP 1 REQUIREO O .O TO MINUTES CPU T IM E » A60 1 .8 2 5 MINUTES CLOCK TIM E______________ ______________________
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 2 CYCLE TIM E 7 5 .0 0 0 0 PAYS TOTAL TIM E 2 2 5 .0 0 0 0 DAYS
ITFftStlO N FLU* CHANCE----------S E T T
IS 3 . lV « 1 3 ? -0 5 1 . 3 :
H I F I ------ RU=2------SHFS—
* .6 2 0 4 2 — 0 .6 0 0 5 6 1 .0 0 5 2 6
X SEARCH FACTOR CROSS SEC TIO N S UPOATEO W ITH 6 .1 9 0 9 0 0 * 0 3 CROSS SE£?t(fti4 U P O A fio W ITH -2 .2 7 C 3 1 0 -0 4
1 .0 0 0 0 0 3 1 .3 3 3 2 7 0 -0 5 _____________________
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF THE R E S ID E S - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 1 0 K 1 .0 0 0 0 0 29
END OF C R IT IC A L IT Y SEARCH - IT E R A T IO N TIM E 0 .0 3 9 M INUTES ______________ _________________________________ _____
IN PU T R E LA TIV E CONCENTRATION CHANGE TIM ES 5 .9 6 3 B 6 E -0 3 HAS BEEN APOEO TO THE I N I T I A L SEARCH CONCENTRATIONS
FRACTIO N A B S O R P TIO N IN SEARCH NUCLIDES- 0 .0 1 8 4 1 4 _____ ______________
LEAKAGE 1.50714E 18 TOTAL LOSSES 1 .1 2 0 6 U E 20 TO TAL PRODUCTIONS 1 .1 2 0 6 0 E 20 REACTOR POhERlWATTS* 2 .5 7 7 3 2 E 09
pose* m m m n w — j ^ 9g gg ; m x i nuM &ESgT T r ~ * . i * r e y8 S '57 ~ In i t * — ~ * r end s u b s te p — I ------------------------------------------------------
AFTER STEP 2 OF CYCLE 2 t THE TIM E IS 1 5 0 .0 0 0 0 OAYS. THE TIM E STEP MAS 7 5 .0 0 0 0 O AYS. ANO TOTAL TIM E IS 3 0 0 .0 0 0 0 DAYS
MULTI-CYCLE BREEDER <S*EA«EO ROCS A D JU S TED . RECYCLE FEED OSTERMINEOI12X8X3 GROUPS* 288 P O IN TS I R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
SUMMARY OF NEUTRON LOSSES, ETC. FOR STEP 2 CYCLE 2 AT CYCLE D EPLETION TIM E 1 1 2 .5 0 OAYS. F IS S IL E KG IS A7 1 5 0 .0 0 OAYS
ZONE CLASS CORE A l
F IS S IL E0 .1 2 5 2 9
F E R TIL E0 .15431
IN TERM EDIATE OTHER STRUCTURAL 0 .0 0 .0 0 0 9 9 0 .0 1 4 3 5
SPECIAL0 .0 0 0 2 6
U N S PEC IFIED0 .0 1 2 5 4
SUMS0 ,3 0 7 7 4
CONV. R A TIO 1 .0 5 0 5 3
POWER1MM1 9 .1 4 7 3 4 E 02
F IS S IL E IK G ) 8 .8 6 8 4 IE 02
Co r e A2 0 .1 2 3 0 7 0 .1 4 3 2 6 0 .0 0 .0 0 0 9 9 0 .0 1 2 8 9 0 .0 0 0 2 2 0 .0 1 1 0 4 0 .2 9 1 4 7 0.9 7 9 6 3 9 .0 5 5 7 2 E 02 9 . 87850E 02CORE A3 0 .0 8 8 1 4 0 .0 9 0 9 6 0 .0 0 .0 0 0 7 1 0 .0 0 8 1 0 0 .0 0 0 1 4 0 .0 0 6 2 2 0 .1 S 4 2 7 0 .8 5 5 6 3 6 .4 5 1 3 5 E 02 . 1 . 12804E 9?BLNk Cl 0 .00*41 0 . 04232 0 .0 0.00001 0 .0 0 3 6 5 0 .0 0 0 1 4 0 .0 0 0 1 3 0 .0 5 0 6 5 9.2 6 4 6 1 3 .5 1 0 5 7 E 01 9 .45435E 01BLNK C2 0 .0 0 3 4 1 0.0 3 6 5 5 0 .0 0.00001 Q .00305 0 .0 0 0 1 0 0 .0 0 0 1 0 0 .0 4 3 2 3 1 0 .3 1 8 5 9 2 .8 5 0 6 7 E 01 8.7 9 8 8 3 E 01BLNK C3 0 ,0 0 X 5 2 0 . 02225 0 , 0 0 ,0 0 0 0 0 0 .0 0 1 8 4 0 .0 0 0 0 6 O.OOOOS 0 .0 2 5 7 1 1 4 .1 5 6 9 0 1 .4 1 5 5 3 E 01 6.3 7 7 9 4 E 01BLNK B l 0 .0 0 3 1 0 0 .0 4 0 1 2 0 .0 0.00000 0 .0 0 2 2 7 0 .0 0 0 0 4 0.00011 0 .0 4 5 6 5 12.3 3 4 2 4 3 .0 9 8 9 6 E 0 } 1 .1 1 6 2 3E 92BLNK B2 0 .00102 0 .0 1 7 7 7 0.0 OeOOOOO 0 .0 0 1 0 3 0 .0 0 0 0 2 0 .0 0 0 0 2 0 .0 1 9 8 6 17.0 5 8 0 4 8 .2 1 8 2 0 E 00 8 . 23572E 01RFLTR E 0.0 0.0 0.0 0 .0 0 .0 0 3 0 2 0 .0 0 0 0 4 0.0 0 .0 0 3 0 6 0 .0 0.0 0.0ftFLTR d 0.0 o.b 0 .0 0.0 6.66i t i 0 .0 0 0 0 8 0.00000 0 .0 0 5 8 1 0.0 0.0 0.0
OTHER LO S S ES ' BASED ON S TA R T-O f -S T E P TOTAL LOSSES 0 .0 1 2 5 5
OVERALL 0 .3 4 9 9 5 0 .5 4 7 5 5 0.0_
0 .0 0 2 7 0 0 .0 5 5 9 3 0 .0 0 1 1 1 0 .0 3 0 2 1 1 .0 0 0 0 0 1 .3 7 3 7 8 2 .5 8 2 4 2 E 03 3 .4 4 3 0 3 E 03
TIM'S STEP THERMAL ENERGY* MW- HRS 4 .6 4 8 3 5 E 06 AND TOTAL. IS 1 .8 5 9 7 5 E 07
T IM E STEP 2 REQUIRED 0 .0 6 7 M INUTES CPU T IM E , AND 1 .3 2 9 M INUTES CLOCK T I M E ______________________________________________
A FIN A L FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 2 TO TA L D EP LETIO N TIM E 3 0 0 .0 0 9 DAYSI t e r a t i o n Fl DX CHAnSE BFT2 B I F I H iF S Bu=3 ic s e a r c h f a c t o r
____________________________________________________________________________________________CROSS SECTIONS UPDATED WITH 5 .0 5 7 7 8 D -0 3 __________________________CrtOSS SECTIO N S UPDATED W ITH -1 .9 5 5 1 9 0 -0 4 #
16 3 .7 i9 3 3 E -0 5 1 .3 9 1 7 4 -0 .4 0 5 1 6 -0 .5 5 8 B 0 1 .0 0 9 2 1 1 .0 0 0 0 0 3 1 .6 6 3 0 6 0 -0 5 IV)------------------------------------------------------------------------------- - CT\CONVERGENCE IN D IC A TIO N BY M IN IM IZIN G THE SUM OF TH E SQUARES OF THE RESIDUES - R E LA TIV E ABSORPTION 1 .0 0 0 0 0 1 0 K 1 .0 0 0 0 0 4 6 CT\
END OF C R I1 IC A L IT Y SEARCH - IT E R A TIO N TIM E 0 .0 4 2 PINUTES_______________________________________________________________________________________________
INPUT R E LA TIV E CONCENTRATION CHANGE T I K -S 4 .8 6 2 2 6 E -0 3 HAS BEEN AOOEO TO THE I N I T I A L SEARCH CONCENTRATIONS__________________________
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 1 9 3 6 6 __________________________________________________________________________________________________________
LEAKAGE 1.54570E 18 TOTAL LOSSES 1 .1 2 0 8 1 E 20 TO TA L PRODUCTIONS 1 .1 2 0 8 1 E 20 REACTOR POhERtW ATTS) 2 .5 7 7 3 2 E 09
12X8X3 GROUPSt 2BB P O IN TS ( R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
FIN A L SUMMARY OF NEUTRON LOSSES* ETC . FOR CYCLE 2 TO TA L D EPLETIO N TIM E 3 0 0 .0 0 OAYS
ZONE CLASS CORE A l
F IS S IL E0 .1 2 6 7 0
F E R TIL E0 .1 5 5 1 0
IN TERM EDIATE OTHER STRUCTURAL 0 .0 0 .0 0 1 0 1 0 .0 1 4 4 9
SPECIAL0.0 0 0 2 7
U N S PEC IFIED0 .0 1 3 7 8
SUMS0 .3 1 1 3 5
CONU. R A TIO 1 .04241
POHERIMU) 9 .2 6 1 4 7 E 02
F I S S I L E U G ) 8 .8 6 8 4 1 E 02
tO R E A2 CORE AH
0 .1 2 1 3 50 .0 8 5 9 9
0 .1 4 0 8 80 .0 8 8 8 5
0 .00 .0
0 .0 0 0 9 80 .0 0 0 7 0
0 .0 1 2 7 30 .0 0 7 9 3
0 .0 0 0 2 20 .0 0 0 1 4
0 .0 1 1 8 50 .0 0 6 5 8
0 .2 8 8 0 10 .1 9 0 1 9
0 .9 7 6 0 90 .8 5 6 6 9
8 .9 3 5 7 2 E 6 .2 9 6 2 8 E
0202
9 .8 7 8 5 0 E1.12804E
0203
BLNK £1 BLNK C2
6 .o o $ lo0 .0 0 3 8 3
0 .0 4 3 5 $0 .0 3 6 7 9
0 .00 .0
0 .0 0 0 0 10 .0 0 0 0 1
0 .0 0 3 7 60 .0 0 3 0 7
0 .0 0 0 1 40 .0 0 0 1 0
0 .0 0 0 1 50 .0 0 0 1 2
0 .0 5 2 7 50 .0 4 3 9 3
8 .2 2 7 9 89 .2 3 6 9 7
4 .0 0 4 2 2 E 3 .1 4 1 4 3 E
0101
9 . 45435E 8 .7 9 8 8 3 E
0101
BLNK C3 BLNK 81
0 .0 0 1 6 60 .0 0 3 3 8
0 . 02215 0 .0 3 9 6 0
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 0
0 .0 0 1 8 30 .0 0 2 2 4
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 50 .0 0 0 1 2
0 .0 2 5 7 50 .0 4 5 3 9
1 2 .8 8 0 6 61 1 .1 6 2 5 2
1 .5 0 9 2 7 E 3 .2 7 4 5 6 E
0101
6 . 3779*E 1 .11623E
0102
BLNK B2 RFLTR E
0 .0 0 1 0 80 .0
0 .0 1 7 6 8 0 .0
0 .00 .0
o .o o o o c0 .0
0 .0 0 1 0 20 .0 0 3 0 2
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 20 .0
0 .0 1 9 8 20 .0 0 3 0 6
16.0 3 3 5 10 .0
ti. 68979 E 0 .0
00 8 .2 3 5 / 2 E0 .0
01
RFLtR 6 A .o 6 .0 0 .0o t h e r
0 .0 0 .0 0 5 8 9 0 .0 0 0 0 8 0 .0 0 0 0 0 LO S SES' BASED ON S T A R T -O F -S TE P TO TA L LOSSES
0 .0 0 5 9 70 .0 1 3 8 0
0 .0 0 .0 0 .0
OVERALL 0 .3 4 9 0 8 0 .5 4 4 6 4 0 .0 0 .0 0 2 7 1 0 .0 5 5 9 8 0 .0 0 1 1 1 0 .0 3 2 6 7 l.O O O O J 1.3 6 8 9 1 2 .5 7 7 3 3 E 03 3 . 443C3E 03
MULTI-CYCLE BREEDER (SMEAREO ROCS ADJUSTED, RECYCLE FEED DETERMINED:12X8X3 GROUPS, 288 POINTS ( R - 2 1 . STREAM OF C I T A T I O N CASES ORNL 72
START FUEL MANAGEMENT FOR CYCLE 2
END FUi MANAGEMENT FOP. CYCLE 2
Cy c l e REQUIRED ’ J . 2 6 4 MINUTES CPU T I M E , AND 5 .1 3 2 MINUTES CLOCK TIME
MU LTI-C Y C LE BREEDER (SHEARED RODS ADJUSTED. RECYCLE FEED DETERMINED)I2XBX3 GROUPS, 288 POINTS ( R - Z ) . STREAM OF C ITATION CASES ORNL 72
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIM E 0 .0 DAYS TOTAL T IN E 3 0 0 .0 0 0 0 DAYS
L IN E RELAXATION W ILL BE DONE ON ROWS AND COLUMNS - 1 INNER IT E R A T IO N !S )_____________________________________________________________________L IM IT IN G VALUES OF THE SEARCH FACTOR FOR A6SORPTION AND TO TA L LOSS ARE -2 .4 6 1 6 8 E 00 -4 .9 1 5 9 3 E 00ITERATION FLUX CHANGE BETA________HU-l________ MU-2________ MU-3________________ K. SEARCH FACTOR____________________________________________
CROSS SECTIONS UPDATED WITH 3.82901D-Q2____________________________________________________________________________________________ CROSS SECTIONS UPDATED WITH -1 .3 5 7 4 0 0 -0 3 ______________________
22 1 .2 7 7 9 2 E -0 4 1 .3 9 1 7 4 -1 .8 7 2 3 6 -1 .6 9 6 3 9 2 .4 1 1 2 4 1 .0 0 0 0 1 1 5 .6 4 7 6 9 D -0 5
Co n vergence i n d ic a t io n by m in im iz in g th e sum o f th e s q u a re s o f th e re s id u e s - r e l a t i v e a b s o r p t io n 1 .0 0 0 0 0 3 8 k 1 .0 0 0 0 0 8 6
ENb OF C R IT IC A L I¥ y StAkCH - ITE R A TIO N TIM E 0 .0 4 2 PINUTES
IN P U T R E LA TIV E CONCENTKATION CHANGE T IK E S 3 .6 9 3 2 7 E -0 2 HAS BEEN ADDED TO THE IN I T I A L SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 2 2 4 7 8
LEAKAGE I . '3178IE 16 TOTAL LOSSES 1 .1 2 0 6 9 E 2C TO TAL PRODUCTIONS 1 .1 2 0 6 9 E 20 REACTOR POWER(WATTS) 2 .S 7 7 3 2 E 09
W J L T I -C YCLE BREEDER (SMEARED RODS ADJUSTED. RECYCLE PEED DETERMINED!12X8X3 CROUPS, 288 POINTS iR -Z I . STREAM OF CITATION CASES ORNL 72
SUM..ARY OF NEUTRON LOSSES, ETC. BEFORE OEPLETING STEP 1 OF CYCLE 3 TOTAL DEPLETION TIME 300,00 OAYS
ZONE CLASS FISSILE FERTILE INTERMEDIATE OTHER STRUCTURAL SPECIAL UNSPECIFIED SUMS CONV, RATIO POWER!MM) FISSILEIKG )CORE A1 3.123 73 0.15247 0 .0 0.00096 0.01410 0.00026 0.01340 0.30492 1,05061 9 .0 4 1 77E 02 8.88929E 02CORE A2 0.12343 0.14313 0 .0 0.00097 0.01281 0.00022 0.01187 0.29243 0,97526 9.08507E 02 9,970305 02CORE A3 0.08947 0.09105 0 .0 0.00071 C .00811 0.00014 0.00690 0.19639 0.84251 6.54324E 02 1.14607E. WBLNK Cl 0.00381 0.04180 0 .0 0.00001 0.00359 0.00014 0.00012 0,04946 10.58113 3.17159E 01 7.36578E 01BLNK C2 0.00299 0.03645 0 .0 0.00000 0.00304 0.00010 0.00009 0.04267 11.75840 2.61494E 01 6 ,9249IE 01BLNK C3 0.00136 0.02233 0 .0 O.OOOCO 0.00185 0.00006 0.00004 0,02564 15.81184 1.33556E 01 5 ,1986£E 01BLNK BI 0.00277 0. 04049 0 .0 0.00000 0.00229 0.00004 0.00011 0.04S70 13.92332 2.93665E 01 9. 06200E 01BLNK 62 0.00126 0.01798 0 .0 0.00000 0.00104 0.00002 0.00003 0,02033 13,96824 9.73456E 00 9 . 37516E 01RFLTR E 0 .0 0 .0 0 .0 0 .0 0.00308 0.00004 0 .0 0.00312 0 ,0 0 .0 0 .0RFLTR D 0 .0 0 .0 0 .0 0 .0 0.00570 O.OOOOu 0.00000 0,00578 0 ,0 0 ,0 0 ,0
OTHER LOSSES * BASED ON START-OF-STEP TOTAL LOSSES 0,01356
OVERALL 0.34882 0.54570 0 .0 0.00266 0.05561 0.00110 0.03256 1,00000 1,37291 2.57733E 03 3.41119E 03
PGWER NORMALIZATION t . 99648, i-.AXlMUH POWER OENSITY 4.595771E 02 IN ZONE 3 AT END SUBSTEP 1
*vi********************************4*«:t***********«***********£***************************«*********************************AFTER STEP 1 OF CYCLE 3 , THE TINE IS 75.0000 DAYS. THE TIME STEP WAS 75.0000 OAYS. AND TOTAL TIHE IS 375.0000 OAYS**************************************************♦**'>*******************,#*******<1***************************************** 2
70
MULTI-CYCLE BREEDER ISMEA.^o apps ADJUSTCD, RECYCLE FEED DETERMINED!12X8X3 GROUPS, 288 P O IN TS i R - Z ) . STREAM OF C IT A T IO N CASES ORNL 72
SUMMARY OF NEUTRON LOSSES* E T C . FOR STEP I CYCLE 3 AT CYCLE DEPLETION T IH E 3 7 .5 0 D AYS. F IS S IL E KG IS AT 7 5 .0 0 OAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 3 8 6
F E R TIL E0.1 5 1 7 5
INTERM EDIATE OTHER STRUCTURAL 0 .0 0 .0 0 0 9 7 0 .0 1 4 1 0
SPECIAL0 .0 0 0 2 6
UN S PECIFIEO0 .0 1 4 0 6
SUMS0 .3 0 5 0 0
CONV. R A TIO 1 ,0 4 4 0 7
POWER!MW> 9 .0 4 6 2 3 E 02
F IS S IL E IK G I 8 .9 1 5 1 4 E 02
CORE A2 0 .1 2 3 2 2 0 .1 4 2 5 3 0 . 0 0 .0 0 0 9 8 0 .0 1 2 8 1 0 .0 0 0 2 2 0 .0 1 2 4 5 0 .2 9 2 2 2 0 .9 7 2 3 9 9.G 6973E 02 9 .9 4 4 2 6 E 02CORE A3 0 .0 8 9 1 0 0 .0 9 0 8 2 0 . 0 0 .0 0 0 7 1 0 .0 0 8 1 1 0 .0 0 0 1 4 0 .0 0 7 1 6 0 .1 9 6 0 5 0 .8 4 3 5 8 6. S I 993E 02 1 . 1372 7E 03&LNK C l 0 .0 0 4 * 4 0 . 04T72 6 . 0 0 .0 0 0 0 1 0 .0 0 3 5 9 0 .0 0 0 1 4 0 .0 0 0 1 3 0 .0 4 9 9 2 9 .2 8 1 0 8 3 .4 5 8 5 3 E 01 9.4 3 6 3 3 E 01BLNK C2 0 .0 0 3 3 8 0 .0 3 6 3 9 0 . 0 0 .0 0 0 0 1 0 .0 0 3 0 4 0 .0 0 0 1 0 0 .0 0 0 1 0 0 .0 4 3 0 2 1 0 .3 8 7 9 3 2 .8 2 7 5 0 E 01 8 .7 5 2 1 IE 01BLNK t3 0 .00151 0.02231 0 . 0 0 .0 0 0 0 0 0 .0 0 1 8 5 0 .0 0 0 0 6 0 .0 0 0 0 5 0 .0 2 5 7 7 1 4 ,2 3 3 9 0 1 .4 1 7 2 4 E 01 6 .3 5 1 6 9 E 01BLNK B l 0 .0 0 3 1 0 0 .0 4 0 4 4 0 . 0 0 .0 0 0 0 0 0 .0 0 2 2 9 0 .0 0 0 0 4 0 .0 0 0 1 2 0 .0 4 5 9 9 1 2 .4 3 8 6 0 3 .1 1 7 4 7 E 01 1 . 10960E 02
■BlNK B2 0.0 0 1 3 2 0 .0 1 * 9 7 <)e6 0 .0 0 0 0 0 0 .0 0 1 0 4 0 .0 0 0 0 2 0 .0 0 0 0 3 0 .0 2 0 3 9 1 3 .2 8 2 6 4 1 .0 0 8 1 3 E 01 1.03122E 02RFLTR E 0 . 0 0 . 0 0 .0 0 .0 0 .0 0 3 0 8 0 .0 0 0 0 4 0 .0 0 .0 0 3 1 2 0 . 0 0 . 0 0 . 0R f l T r 6 0 . 6 6 .6 0 . 0 6 .0 0 .6 0 5 7 0 0 .0 0 0 0 8 0 .0 0 0 0 0 0 .0 0 5 7 8 0 . 0 0 . 0 0 . 0
OTHER LOSSES* BASED ON STAR T-O F -S T E P TO TAL LOSSES 0 .0 1 2 7 5
OVERALL 0 .3 4 9 8 2 0.5 4 3 9 3 0 .0 0 .0 0 2 6 9 0 .0 5 5 6 1 0 .0 0 1 1 0 0 .0 3 4 1 0 1 .0 0 0 0 0 1 .3 6 4 2 2 2 .5 8 1 8 8 E 03 3 .4 8 2 6 9E 03
TIM E STEP THERMAL ENERGY, MW- HRS 4 .6 4 7 3 8 E 06 AND TOTAL IS 2 .3 2 4 4 9 E 07
TIM E STEP I REQUIRED 0 .0 7 1 MINUTES CPU T IM E , AND 0 .6 6 5 MINUTES CLOCK TIM E____________________________________________________________
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE CYCLE T IM E 7 5 .0 0 0 0 DAYS TO TA L TIM E 3 7 5 .0 0 0 0 DAYS__________________________
I t e r a t i o n F l u x c h a n g e b e t a hlF I miF 2 mT F 3 k s e a r c h f a c t o r____________________________________________________________________________________________ CROSS SECTIONS UPDATED WITH 3 .* 0 5 3 1 0 -0 3 ______________________
CROSS SECTIO NS UPDATED H ITH -1 .1 8 6 0 6 D -0 415________ 2 .9 5 6 3 9 E -0 5 1 .3 9 1 7 4 -0 .4 4 2 4 3 -0 ,4 5 7 9 3 1 .00437________ 1 .0 0 0 0 0 2 1 .3 2 2 2 4 0 -0 5 _____________________________________________
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIOUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 1 0 K 1 .00 0 0 0 3 B
END OF C R IT IC A L IT Y SEARCH - ITE R A TIO N TIM E 0 .0 3 7 PINUTES___________________________________________________________________________________________
INPUT R E LA TIV E CONCENTRATION CHANGE TIM ES 3 .2 8 6 7 1 E -0 3 HAS BEEN ADDED TO THE IN I T I A L SEARCH CONCENTRATIONS______________________
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 2 3 0 7 3 ______________________________________________________________________________________________________
LEAKAGE 1.55651E 18 TOTAL LOSSES 1 .1 2 0 9 0 E 20 TO TA L PRODUCTIONS 1 .1 2 0 9 0 E 20 REACTOR POWER!WATTS) 2 .5 7 7 3 2 E 09
Powtft NdftMALtZATlQN 6 .9 9 6 7 ? , MAXIMUM f>OWER D E N S ltY 4 .6 2 9 1 8 9 E 02 IN ZONE 1 AT END SUBSTEP T
***************************************it***********************************************************************************AFTER STEP 2 OF CYCLE 3 , THE T IH E I S 1 5 0 .0 0 0 0 OAYS. THE TIM E STEP WAS 7 5 .0 0 0 0 DAYS, AND TO TAL TIM E IS 4 5 0 .0 0 0 0 DAYS ****************************************************************************************************************************
27
1
MULTI-CYCLE BREEDER tSMEAREO RODS AOJUSTEO. RECYCLE FEED DETERMINED)12X8X3 GROUPS, 288 P O IN TS I R - 2 ) . STREAM OF C IT A T IO N CASES Cfi.JI. .2
SUMMARY OF NEUTRON LOSSES* E T C . FOR STEP 2 CYCLE 3 AT CYCLE DEPLETION T IN E 1 1 2 .5 0 OAYS. F IS S IL E KG I AT 1 5 0 .0 0 OAYS
ZONE CLASS F IS S IL E F E R TIL E IN TERM EDIATE OTHER STRUCTURAL SPECIAL U N S PEC IFIED SvJMS CONV. R A TIO POWER!MW) F IS S IL E IK G 1:ORE AL 0 .1 2 5 3 9 0 .1 5 1 9 4 0 .0 0 .0 0 1 0 0 0 .0 1 4 2 5 0 .0 0 0 2 6 0.0 1 5 8 2 0 .3 0 8 6 5 1.0 3 0 4 6 9 .1 6 4 0 4 E 02 8 . 93 I6 7 E 0?,tORE A2 ' 0 .1 2 1 3 3 0 .1 3 9 6 9 0 .0 0 .0 0 0 9 9 0 .0 1 2 6 6 0 .0 0 0 2 2 0 .0 1 3 6 8 0 .2 8 8 5 5 0 .9 6 6 5 6 8.9 3 6 7 9 E 02 9 .91461E rt 9CORE A3 0 .0 8 6 6 1 0 .0 8 8 5 4 0 .0 0 .0 0 0 7 1 0 .0 0 7 9 5 0 .0 0 0 1 4 0 .0 0 7 6 8 0 .1 9 1 6 3 0 .8 4 5 9 2 6 .3 4 2 9 6 E 02 1 . 1288 2E v.3fkLNK Cl 0 .0 0 5 5 5 0 .0 4 2 9 0 0 .0 0.0 0 0 0 1 0 .0 0 3 7 0 0 .0 0 0 1 4 0 .0 0 0 1 8 0 .0 5 2 4 8 7 .44172 4 .2 3 4 6 8 E 01 1 .14976E -2BLNK C2 0 .0 0 4 1 7 0 .0 3 6 5 9 0 .0 0 .0 0 0 0 1 0 .0 0 3 0 6 0 .0 0 0 1 0 0 .0 0 0 1 3 0.C44O 7 6 .4 3 3 2 5 3 .3 2 ? -siSE 02BLNK C3 0 .0 0 1 8 0 0 .0 2 2 2 0 0 .0 0.00000 0 .0 0 1 8 4 0 .0 0 0 0 6 0 .0 0 0 0 5 0 .0 2 5 9 5 1 1 .8 8 4 3 0 1 .5 9 1 c E 01 7 . 48075E 01BLNK BX 0 .0 0 3 6 9 0 .8 3 ^ 8 9 0 .0 0 ,0 0 0 0 1 0 .0 0 2 2 6 0 .0 0 0 0 4 0 .0 0 0 1 4 0 .0 4 6 0 3 1 0.27986 3 .4 7 0 ^ --E 01 1 . 3073QE 02BLNK B2 0 .0 0 1 4 4 0 .0 1 7 8 8 0 .0 0.00000 0 .0 0 1 0 4 0 .0 0 0 0 2 0 .0 0 0 0 3 0 .0 2 0 4 2 12.09615 1 .0 8 9 E 01 1 . 12362E 02RFLTR E 0 .0 0 .0 0 .0 0 .0 0 .0 0 3 0 B 0 .0 0 0 0 4 0 .0 0 .0 0 3 1 2 0 .0 0 .0 0 .0Rft.TR d 0 .0 0 .0 0 .0 0 .0 0 .0 0 5 8 6 0 .0 0 0 0 8 0 .0 0 .0 0 5 9 4 0 ,0 0 .0 0 .0
OTHER LOSSES* BASED ON S T A R T -O F -S TE P TOTAL LOSSES 0 .0 1 3 1 6
OVERALL 0 .3 4 9 9 8 0.53963 0 .0 0 .0 0 2 7 3 0 .0 5 5 6 9 0 .0 0 1 1 1 0 .0 3 7 7 1 1 .0 0 0 0 0 1 .35161 2 .5 8 1 5 0 E 03 3.55173E 03
TIM E STEP THERMAL ENERGY, MW-HRS 4 .6 4 6 7 0 E 06 AND TOTAL IS 2 .7 8 9 1 6 E 07
T IH E STEP 2 REQUIRED 0 .0 6 5 H IN U TES CPU T IM E . AND 0 .6 3 3 MINUTES CLOCK TIM E
A FIN A L FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 TO TAL DEPLETION TIM E 4 5 0 .0 0 0 DAYSI t E r a T I o n f*LUx change b e ta to u -i mu- 2 m u-3 K SEARCH FACTOR
CROSS SECTIONS UPDATED WITH 2 .3 8 4 8 8 0 -0 3
15 2 .3 8 4 1 9 E -0 5 1 .3 9 1 7 4 -0 .4 3 2 4 1 -0 .7 3 5 4 4 0 .8 6 5 5 1CROSS SECTIONS UPDATED WITH
1 .0 0 0 0 0 2 9 .7 1 2 9 3 0 -0 6-6 .8 7 3 1 8 0 — 05
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 1 .0000000 K 1 .000 0 0 3 8
END OF C R I T I C A L L Y SEARCH - ITE R A TIO N TIM E 0 .0 4 2 MINUTES
INPUT R E LA TIV E CONCENTRATION CHANGE TIM ES 2 .3 1 6 1 5 E -0 3 HAS BEEN AODEO TO THE I N I T I A L SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 2 3 4 5 8
LEAKAGE 1.59676E IB TO TAL LOSSES 1 .1210B E 20 TO TA L PRODUCTIONS L.121G8E 20 REACTOR POtaERlWATTS) 2 .5 7 7 3 2 E 09
*
MULTI-CYCLE BREEDER ( SHEARED ROCS ADJUSTED, RECYCLE FEED DETERMINED)12X8X3 GROUPS, 288 POINTS (R - 2 1 . STREAM OF C I T A T IO N CASES ORNL 72
FIN A L SUMMARY OF NEUTRON LOSSES, E T C . FOR CYCLE 3 TO TAL D EPLETION T IH E 4 5 0 .0 0 OAYS
ZONE CLASS CORE A I
F IS S IL E0 .1 2 6 5 9
F E R TIL E0 .1 5 2 5 9
IN TERM EDIATE0 .0
OTHER STRUCTURAL 0 .0 0 1 0 2 0 .0 1 4 3 7
SPECIAL0 .0 0 0 2 7
UN S PECIFIED0 .0 1 6 8 3
SUMS0 .3 1 1 6 6
CONV. R A TI3 1 .0 2 3 5 6
POWERiKHl 9 .2 6 1 5 2 E 02
F I3 S IL E < KG) 8 .9 3 1 6 7 E 02
CORE A2 CORE A3
0 .1 1 9 7 *0 .0 8 4 6 8
0 .1 3 7 5 6 0 .0 8 6 7 0
0 .00 .0
0 .0 0 0 9 90 .0 0 0 7 0
0 .0 1 2 5 10 .0 0 7 8 1
0 .0 0 0 2 20 .0 0 0 1 4
0 .0 1 4 2 40 .0 0 7 8 9
0 .2 8 5 2 60 .1 8 7 9 1
0 .9 6 3 6 70 .8 4 7 1 9
8 .8 2 5 5 6 E6 .2 0 3 6 9 E
0202
9 .9 1 4 6 1 E1.1 2 8 8 2 E
0203
&LNK C l BLNK C2
0 .0 0 6 2 60 .0 0 4 5 9
0 . 04414 0 .0 3 6 8 7
0 .00 .0
0 .0 0 0 0 10 .0 0 0 0 1
0 .0 0 3 8 10 .0 0 3 0 9
0 .0 0 0 1 40 .0 0 0 1 1
0.0 0 0 2 10 .0 0 0 1 5
0 .0 5 4 5 80 .0 4 4 8 0
6 .7 6 6 '7 7 .7 1 1 6 6
4 .7 4 3 5 4 E3 .6 I6 8 0 E
0101
1 . 14976E 1 .05409E
0202
BLNK C3 BLNK 81
0 .0 0 1 9 40 .0 0 3 9 6
0 . 02214 0 .0 3 9 4 7
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 1
0 .0 0 1 8 30 .0 0 2 2 4
0.0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 60*00014
0 .0 2 6 0 30 .0 4 5 8 5
1 0 .9 8 6 7 49 .4 7 1 6 6
1 .6 8 5 6 9 E3 .6 4 2 5 2 6
01Oi
7 .4 8 0 7 5 E1 .3 0 7 3 0 c
0102
BLNK 62 RFLTR E
0 .0 0 1 5 00 .0
0 .0 1 7 8 30 .0
0 .00 .0
0 .0 0 0 0 00 .0
0 .0 0 1 0 30 .0 0 3 0 9
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 40 .0
0 .0 2 0 4 20 .0 0 3 1 3
1 1.579420 .0
1.1 3 6 8 2 E0 .0
01 1.12362E0 .0
02
u n r " ■ - 0 .0 0 .0OTHER LOSSES
0 .0 0 .0 0 6 0 3 0 .0 0 0 0 8 0 .0 • BASED ON S T A R T-O F -S TE P TO TA L LOSSES
0 .0 0 6 1 10 .0 1 4 2 5
0 .0 0 .0 0 .0
OVERALL 0 .3 4 9 2 6 0.5 3 7 2 9 0 .0 0 .0 0 2 7 4 0 .0 5 5 8 0 0 .0 0 1 1 1 0 .0 3 9 5 5 1 .0 0 0 0 0 1 .3 4 7 6 4 2 .5 7 7 3 3 E 03 3 . 55173E 03
REPEAT CYCLE CONVERGENCE IS >8 . 88779E— 01
REPEATING CYCLE 3 ITE R A TIO N NUMBER 1
MULTI-CYCLE BREEDER £ SHEARED ROCS ADJUSTED, RECrCLE FEtEO OETERHINEOI12X8X3 GROUPS, 288 P O IN TS ( R - Z ) . STREAM OF C IT A T IO N CASES ORNL 72
SfA R t hJEL mAnAGe H6n t f o r Cy c l e 2
THE FACTOR APPLIED TO THE RECYCLE FRACTIO N FOR REPEAT CYCLE IS 9 .0 0 0 0 0 E -0 1
END FUEL MANAGEMENT FOR CYCLE 2
MULTI-CYCLE BREEDER (SMEARED RODS ADJUSTED, RECYCLE FEED DETERMINED!12X8X3 GROUPS, 288 POINTS IR -Z I . STREAM OF CITATION CASES ORNL 72
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIME oTo DAYS TOTAL TIME 300.0000 OAYS
LINE RELAXATION HILL BE DONE ON ROWS AND COLUMNS - 1 INNER ITERATIO NS!_____________________________________________________________________LIMITING VALUES OF THE SEARCH FACTOR FOR ABSORPTION AND TOTAL LOSS ARE -2.43633E 00 -4.89376E 00ITERATION FLUX CHANGE BETA________ MU-1________ MU-2 MU-3________________ K SEARCH FACTOR____________________________________________
CROSS SECTIONS UPDATED *ITH -4.19201D-02____________________________________________________________________________________________ CROSS SECTIONS UPDATED WITH 1,333480-03______________________
23 —1 .18315E-04 1.39174 -2 ,06783 -1 .66158 3.08830 0.999988 -5 .355460-05
CONVERGENCE INDICATION BY MINIMIZING THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 0.9999946 K 0.9999922
END OF C h lT ltA L IT Y 5£ARCH - ITERATION TIME 0.042 PINUTES
INPUT RELATIVE CONCENTRATION CHANGE TIMES -4 .05867E-02 HAS BEEN ADDED TO THE IN IT IAL SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0.005870
LEAKAGE I.53634S 18 TOTAL LOSSES 1.3.20226 20 TOTAL PRODUCTIONS 1.12022E 20 REACTOR POhER(MATTS) 2 .57 732E 09
MULTI-CYCLE BREEDER (SHEARED RODS ADJUSTED. RECYCLE FEED DETERMINED)12X8X3 GROUPS. 288 POINTS ( R - Z ) . STREAM OF C ITA TIO N CASES ORNL 72
SUMMARY OF NEUTRON LOSSES, ETC. BEFORE DEPLETING STEP I OF CYCLE 3 TOTAL DEPLETION TINE 300 .00 CAYS
ZONE CLASS CORE AI
FISSILE0.12561
FERTILE0.15861
INTERMEDIATE OTHER STRUCTURAL 0 .0 0.00097 0.01475
SPECIAL0.C0027
UNSPECIFIED0.00674
SUMS0.30696
CONV. RATIO POMER(KH) 1.08142 9.15341E 02
FISSILE (KG ) 8.67023E 02
CORE A2 CORE A3
0.123190.08854
0.146400.09231
0 .0 0.00097 0 .0 0.00070
0.013160.00828
0.000230.00014
0.00596O.OOj IB
0 .2 8994 0.19315
1.00429 0.86782
9.04351E6.45729E
02Of?
9.71977E1.11669E
0203
0LNK Cl BLNK C?
0.003940.00304
0.043210.03716
0 .0 0.00001 0 .0 0.^0000
0.003720.00310
0.000140.00011
0.000120.00009
0 .0511*0.04351
10.5840111.76368
3.26690E2.65392E
0101
7.36578E6.92491c
0101
BLNK C3 BLNK B1
0.001380.00280
0.02261 0.04090
0 .0 0.00000 0 .0 0.00000
0.001870.00231
0.000060.00004
0.000040.00011
0.025960.04616
15.8195113.93439
1.34462E2.94783E
0101
5 . 19862E 9.05200E
0101
BLNK B2 RFLTR E
0.001270 .0
0.01810 0 .0
0 .0 0,00000 0 .0 0 .0 .
0.001050.00309
0.000020.00004
0.000030.0
0.020460.00313
13.973340 .0
9.77479E0 .0
00 9.37516E 0 .0
01
Rfi.TR d 0 .0 0 .0 0 .0 0 .0 0.00581 0.00008 0.00000 OTHER LOSSES* BASED ON START-OF-STEP TOTAL LOSSES
0.005890.01370
0.0 0 .0 0 .0
»a ■— _ _ — _ r m_ — — ! ,OVERALL 0.34977 0.55930 0 .0 0.00266 0.05716 0.00113 0.01627 1.00000 1.40785 2 . 57733E 03 3.33485E 03
POWER NORMALIZATION 0.99472. MAXIMUM POWER DENSITY 4.647905E 02 IN ZONE 1 AT END SUdSfEP 1
****4***^t*t~t***t*t*i4t***44***********«******ii***********************************.********rt********************************AFTER STEP I OF CYCLE 3 . THE TIME IS 75.0000 OAYS. THE TIME STEP HAS 7S.QOOO DAYS, AND TOTAL TIME IS 375.0000 DAYS ***********«<**************************************************************;:•*******************#*»**#*********************** rc
- jCT\
HULTI -CV C LE BREEDER ISMEARED RODS ADJUSTgp, RECYCLE FEED OETERM1NED)12X8X3 GROUPS, 288 POINTS IR -Z I . STREAM OF CITATION CASES ORNL 72
SUMMARY OF NEUTRON LOSSESir ETC. FOR STEP 1 CYCLE 3 AT CYCLE OEPLETION TINE 37.50 OAYS. FISSILE KG IS AT 75.00 DAYS
ZONE CLASS CORE A l
FISSILE0.12590
FERTILE0.15783
INTERMEDIATE OTHER STRUCTURAL SPECIAL 0 .0 0.00098 0.01475 0.00027
UNSPECIFIED0.00744
SUHS0.30718
CONV. RATIO POWER*KH) 1.07308 9.16721E 02
FISSILE (KG ) 8.71776E OZ
CORE A2 CORE A3
0.123110.08821
0.145780.09207
0 .0o .g
0.000960.00070
0.013180.00828
0.000230.00014
0.006560.00344
0.289830.19286
1 .0 0 0 2 30.86843
9.C3538E6.43696E
0202
9.71367E I . 10925E
020*
BLNK Cl BLNK C2
0 j00450 0.00345
0.04313 0.03710
0 .00 .0
0.000010.00001
0.003720.00310
0 .0 0 0 14 0.00011
9.00014 a .o o o n
0 .0 5 1 6 30.04386
9.2450310.34880
3.57332E2.S7464E
0101
9. 505C9C S.78725E
0101
BLNK C3 BLNK B l
0.001530.00313
0 .0 2 2 5 80.04085
0.00 .0
0.000000.00000
Q.G0187 0 .00 231
0.0 0 0 0 60.00004
O.uOOOS0.00012
0.0 2 6 1 00.04646
1 4 .2 2 2 9 012.43514
1 .4 2 8 2 7 E3 .13203E
0101
6 .3 6 5 9 0 E1.11167E
0102
BLNK B2 RFLTR E
0.001330 .0
0.018090.0
0 .00 .0
0.000000.0
0.001050.00309
0.00002 Oc00004
0 .0 0 0 0 30 .0
0 .0 2 0 5 20.00313
1 3 .2 8 3 6 00 .0
1 .0 1 2 5 5 E0 .0
01 U 0 3 1 8 0 E0 .0
02
ftfLTR 0 0 .0 0.0 0 .0OTHER
0.0 0.00561 0.00008 0.00000 LOSSES* BASED ON START-CF-STEP TOTAL LOSSES
0 .0 0 5 8 90.01254
0 .0 o .o 0 .0_____ __ — — — _ .ri __m , _ .
OVERALL 0.35117 0.55743 0 .0 0.00269 0.05716 0.00113 0.01788 1 .0 0 0 0 0 1.39720 2.58416E 03 3.41332E 03
TIME STEP THERHAL ENERGY. MU- HRS 4.65149E 06 AND TOTAL IS 2.32490E 07
TIME STEP 1 REQUIRED 0.070 MINUTES CPU TIME* ANO 0.654 MINUTES CLOCK TIHE
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIME 75.0000 DAYS TOTAL TIME 375.0000 OAYS
ITERATION FLUX CHANGE BETA MU-l MU-2 MU-3 K SEARCH FACTOR CROSS SECTIONS UPDATED WITH 1.039880-02
19 4 . 29153E-05 1.39174 -0 .43343 -1 .0 1 6 1 0 0.94554CROSS SECTIONS UPDATED MITH -3 .687680-04
1.000005 2.277140-05
CONVERGENCE INDICATION BY MINIMIZING THE SUM OF THE SQUARES OF THE RESIDUES - RELATIVE ABSORPTION 1.0000019 K 1.0000057
END OF CR 1T.ICALITY SEARCH - ITERATION TIHE 0.041 MINUTES
INPUT RELATIVE CONCENTRATION CHANGE TIMES 1.00300e-02 HAS BEEN ADDED TO THE IN IT IA L SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 0 8 0 6 5
LEAKAGE 1.57356E 18 TOTAL LOSSES 1.12047E 2C TOTAL PRODUCTIONS l.U '0 4 7 E 20 REACTOR POUERIHATTS) 2.57I32E 09
PfiMEft NORMALIZATION 0~.4Q521, MAXIMUM f>OHER DENSITY 4.700334E 02 IN ZONE 1 AT END SUB STEP 1
'4pta***C***?*****a*********************4i**6**i***** ********* **********************************************************AFTER STEP 2 OF CYCLE 3 , THE TIHE IS 150.0000 PAYS. THE T?tHE STfr» Ht.S 75.0000 DAYS. ANO TOTAL TIKE IS 450.0000 DAYS *******4’**4>k****4'*t** ************ *****4 4********** * **4*4*4* * i* * * * i* «* * * * * * * * * a * * * * * * ***************************** ****•••*»*•
277
12X8X3 GROUPS, 288 PO IN TS I R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
SUffflARV TJF n e u t r o n l o s s e s . E T C . FOR STEP 2 CYCLE 3 AT CYCLE DEPLETION TIM E 1 1 2 .5 0 OAYS. F IS S IL E KG IS AT 1 5 0 .0 0 OAYS
ZONE CLASS CORE At
F IS S IL E0 .1 2 7 5 8
F E R TIL E0 .1 5 7 7 2
IN TERM ED IATE OTHER STRUCTURAL SPECIAL 0 .0 0 .0 0 1 0 2 0 .0 1 * 8 8 0 .0 0 0 2 7
UN S PECIFIED0 .0 0 9 8 7
SUMS0 .3 1 1 3 3
CONV. R A TIO 1 .0 5 5 5 7
POmER(MN) 9*29739E 02
F IS S IL S (K G ) 8 .7 5 3 2 6 E 02
CORE A2 CORE A3
0 .1 2 1 1 10 .0 8 5 5 1
0 .1 * 2 * 2 0 .0 6 9 * 2
0 .00 .0
0 .0 0 0 9 90 .0 0 0 7 0
0 .0 1 2 9 80 .0 0 8 0 8
0 .0 0 0 2 20 .0 0 0 1 *
0 .0 0 8 * 10 .0 0 * 3 5
0 .2 8 6 1 10 .1 8 8 1 9
0.9 9 1 7 20 .8 6 9 5 9
8 .8 9 6 2 9 E6 .2 * 6 1 * E
0202
9 .7 0 1 7 7 E 02 1 .10209E 03
BLNK C l BLNK C2
0 .0 0 5 7 90 .0 0 * 2 7
0 .0 * * 3 3 0 .0 3 7 2 2
0 .00 .0
0 .0 0 0 0 10 .0 0 0 0 1
0 .0 0 3 8 30 .0 0 3 1 2
0 .0 0 0 1 *0 .0 0 0 1 1
0 .0 0 0 1 90 .0 0 0 1 3
0 .0 5 * 2 80 .0 * * 8 5
7 .3 7 0 3 08 .3 9 2 1 9
* .3 9 6 9 1 E 3.3B 5Q 4E
0101
1 .1 6 3 1 2E 1.06057E
0202
BLNK C3 BLNK B1
0 .001820 .0 0 3 7 2
0 .0 2 2 * 00 .0 * (ft 5
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 1
0 .0 0 1 8 60 .0 0 2 2 8
0 .0 0 0 0 60 .0 0 0 0 *
0 .0 0 0 0 50 .0 0 0 1 *
0 .0 2 6 2 00 .0 * 6 3 3
11.8 5 6 2 *1 0 .2 6 3 9 8
1 .6 0 1 9 7 E3 .* 7 9 4 8 E
0101
7* 5051*E 1 .3 1 0 6 1 F
0102
BLNK B2 RFLTR B
0 .0 0 1 * 50 .0
0 .0 1 7 9 *0 .0
0 .00 .0
0 .0 0 0 0 00 .0
0 .0 0 1 0 *0 .0 0 3 0 8
0 .0 0 0 0 20 .0 0 0 0 *
0 .0 0 0 0 30 .0
0 .0 2 0 * 80 .0 0 3 1 3
12.0 9 2 5 *0 .0
1 .0 9 1 2 3 E 0 .0
01 1 . 12**6E 0 .0
02
RFLTR d 0 .0 0 .0 0 .0 0 .0 0 .0 0 5 9 7 0*00008 0 .0 0 0 0 0 OTHER LOSSES* BASEO ON S T A R T -O F -S TE P TOTAL LOSSES
0 .0 0 6 0 50 .0 1 3 0 1
0 .0 0 .0 0 .0
OVERALL 0 .3 5 1 2 5 0 .5 5 1 5 9 0 .0 0 .0 0 2 7 3 0 .0 5 7 1 1 0 .0 0 1 1 3 0 .0 2 3 1 7 1.0 0 0 0 0 1 .3 8 0 6 * 2 .5 8 3 5 3 E 03 3 .* 8 8 5 2 E 03
TIM E STEP THERMAL ENERGY* MM-HRS * .6 5 0 3 5 E 06 AND TOTAL IS 2.7 8 9 9 3 E 07
TIM E STEP 2 REQUIRED 0 .0 6 7 MINUTES CPU T IM S , AND 0 .6 3 6 MINUTES CLOCK TIM E____________________________________________________________
A F IN A L FLU* - EIGENVALUE PROBLEM FOLLOWS FOR C YCLE 3 TO TA L O EPLETIO N TIM E * 5 0 .0 0 0 DAYSIT e r a t I O n f l u x cMange BETS H U -i JH F2 S IP S k s e a rc h f a c t o r
________________________________ ____________________________________________________________CROSS SECTIO N S UPDATED WITH 8 .8 2 7 1 9 D -0 3 ______________________CROSS SECTIONS UPDATED WITH -3 .2 3 3 9 3 0 -0 *
19________ 3 .4 3 3 2 3 E -0 5 1 .3 9 1 7 * -0 .3 9 6 9 3 -1 .1 0 2 1 1 0 .9 6 9 6 *________ 1 .0 0 0 0 0 * 2 .1 3 1 6 9 0 -0 S _____________________________________________
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF TH E SQUARES OF THE RESIOUES - R E LA TIV E ABSORPTION 1 .000 0 0 1 9 K 1 .00 0 0 0 5 7
END OF C R 1 T IC A L IT Y SEARCH - IT E R A TIO N TIM E 0 .0 * 1 MINUTES___________________________________________________________________________________________
INPUT R E LA TIV E CONCENTRATION CHANGE TIM ES B .5 0 3 7 9 E -0 3 HAS eEEN ADDEC TO THE I N I T I A L SEARCH CONCENTRATIONS______________________
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 0 9 8 9 0 ________________________________________________________________________ ____________ ______
LEAKAGE 1.6127*E 18 TOTAL LOSSES 1 .1 2 0 7 0 E 20 TOTAL PRODUCTIONS 1 .1 2 0 7 0 E 20 REACTOR P0H ERIHAITS> 2 .S 7 7 3 2 E 09
M U LTI-C Y C LE BREEDER (SMEAREO ROCS AD JUS TED . RECYCLE FEED DETERMINED}12X8X3 GROUPS. 286 PO INTS IR - Z > . STREAM OF C IT A T IO N CASES ORNL 72
F IN A L SUMMARY OF NEUTRON LO S SES. E T C . FOR CYCLE 3 TO TAL D EPLETIO N TIM E 4 5 0 .0 0 OAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 8 7 3
F E R TIL E0 .1 5 8 0 7
IN TERM EDIATE 0 .0 '
OTHER STRUCTURAL 0 .0 0 1 0 4 0 .0 1 4 9 7
SPECIAL0 .0 0 0 2 8
UKSPEC1F1ED0 .0 1 1 4 4
SUMS0 .3 1 4 5 3
CONV. R A TIO 1 .0 4 6 6 4
POWER!MM) 9 .3 9 3 9 0 E 02
F IS S IL E (K G ) 8 .7 5 3 2 6 E 02
CORE A2 CORE A3
0 .1 1 9 3 70 .0 8 3 3 9
G. 13990 0 .0 8 7 2 8
0 .00 .0
0 .0 0 0 9 80 .0 0 0 6 8
0 .0 1 2 8 00 .0 0 7 9 1
0 .0 0 0 2 20 .0 0 0 1 4
0 .0 0 9 5 20 .0 0 4 9 0
0 .2 8 2 7 90 .1 8 4 3 1
0 .9 8 7 3 90 .8 7 0 1 6
B .7 7 5 60 E6 .0 9 5 0 7 E
0202
9.7 0 1 7 7 E 02 1 .1 0 2 0 9 E 03
BLNK C l BLNK C2
0 .0 0 6 ^ 40 .0 0 4 6 9
A.6455>0 .0 3 7 4 4
0 .00 ,0
0 .0 0 0 0 10 .0 0 0 0 1
0 .0 0 3 9 40 .0 0 3 1 3
0 .0 0 0 1 5o .o o c " ::
0 .0 0 0 2 20 .0 0 0 1 5
0 .0 5 6 4 30 .0 4 5 5 3
6 .6 8 7 6 57 .6 6 6 3 1
4 .9 3 2 9 5 E 3 .6 7 9 9 3 E
0101
1 . 16312E 1 .0 6 0 5 7 E
0202
BLNK C3 BLNK B1
0 .0 0 1 9 60 .0 0 3 9 8
0 .0 2 2 2 9 0 .0 3 9 6 0
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 1
0 .0 0 1 8 50 .0 0 2 2 5
0.0C. 96 0 .0 0 0 0 4
0 .0 0 0 0 60 .0 0 0 1 5
0 .0 2 6 2 10 .0 4 6 0 2
1 0 .9 5 5 5 89 .4 5 3 8 4
1 .6 9 3 8 6 E 3 .6 4 4 3 6 E
0101
7 . 50514E 1 .3 1 0 6 IE
0102
BLNK B i RFLTR E
0 .0 0 1 5 00 .0
0 .0 1 7 8 40 .0
0 .00 .0
0 .0 0 0 0 00 .0
0 .0 0 1 0 30 .0 0 3 0 8
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 40.0
0 .0 2 0 4 30 .0 0 3 1 3
1 1 .5 7 4 8 70.0
1 .1 3 6 0 2 E0.0
01 1 . 12446E 0.0
02
RFLfft b 0 .4 0.6 0 .0 0 .0 0 .0 0 6 1 4 0 .0 0 0 0 8 0 .0 OTHER LOSSES* BASED ON S T A R T-O F -S TE P TO TA L LOSSES
0 .0 0 6 2 20 .0 1 4 4 0
0.0 0.0 0.0
■ II ■OVERALL 0 .3 5 0 1 7 0 .5 4 7 9 9 0 .0 0 .0 0 2 7 3 0 .0 5 7 1 0 0 .0 0 1 1 4 0 .0 2 6 4 7 1.00000 1 .3 7 4 7 2 2 .5 7 7 3 3 E 03 3 .4 8 8 5 2 E 03
REPEAT CYCLE CONVERGENCE IS - 5 .7 4 1 3 1 E -0 1
REPEATING CYCLE 3 ITE R A TIO N NUMBER 2
MULTI-CYCLE BREEDER (SHEARED RODS ADJUSTED# RECYCLE FEED DETERMINED)12X8X3 GROUPS, 288 P O IN TS I f t - Z I . STREAM OF C IT A T IO N CASES ORNL 72
" '5 T M T FUEL MANAGEMENT fflk CVCLE
f H i FACtOR APPLIED tO THE RECYCLE FR ACTIO N FOR REPEAT CYCLE IS 8 .7 9 7 0 6 E -0 1
ENi) FUEL MANAGtMENt FOR CYCLE 2
H U L T i-C Y C L E BREEDER (SMEARED RODS A D JU S TED , RECYCLE FEED DETERMINED)12X8X3 GROUPS, 288 PO IN TS I R - Z ) . STREAM OF C itA T IO N CASES ORNL 72
A F lu x - § Id £ kvA Lu£ p R d e t£ M "T0L L 0 w$ F o r C y C le 3 c y c le tim e 0 . 0 days TO TAL TIM E 3 0 0 .0 0 0 0 DAYS
L IN E RELAXATION H IL L BE DONE ON ROWS AND COLUMNS - I INNER IT E R A T IO N (S )L IM IT IN G VALUES OF THE SEARCH FACTOR FOR ABSORPTION AND TO TA L LOSS ARE -2 .4 3 1 1 9 E OO -4 .8 B 9 2 6 E 00ITE R A TIO N FLUX CHANGE BETA MU-1 THJ-2 MU-3 K SEARCH FACTOR
. CROSS SECTIONS UPDATED WITH -5 .7 8 9 6 1 D -0 2CROSS SECTIO NS UPDATED W ITH 1 .8 0 5 3 0 D -0 3
23 -1 .5 9 7 4 0 E -0 4 1 .3 9 1 7 4 - I . 99421 -1 .6 3 0 4 5 2 .9 3 6 2 8 0 .9 9 9 9 8 4 -7 .1 9 1 7 1 0 -0 5
CONVERGENCE IN D IC A TIO N BV M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 0 .9 9 9 9 9 2 9 K 0 .9 9 9 9 8 9 0
END OF C R IT IC A L IT Y SEARCH - ITE R A TIO N TIM E 0 .0 4 9 MINUTES
INPUT R E LA TIV E CONCENTRATION CHANGE TIM ES -5 .6 0 9 0 8 E -0 2 HAS BEEN ADDED TO THE I N IT IA L SEARCH CONCENTRATIONS
FR ACTIO N ABSORPTION IN SEARCH NUCLIDES 0 .0 0 2 3 9 5
Leakage r75TOT5FT8 fdVAL lo s s e s i . i z o i 2 E zo t o t a l p rod u ction s 1 . 12 0 12E 20 r e a c to r p o n e r (h a t ts ) 2 . 57732E 09
M U LTI-C Y C LE BREEDER tSHEARED RODS AD JUS TED , RECYCLE FEED DETERM INED)12X8X3 CROUPS, 288 PO IN TS ( R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
Summary o f n e u t r o n 1 LOSSES, E T C . BEFORE O EPLETIN G STEP 1 OF CYCLE 3 TOTAL DEPLETION TIM E 3 0 0 . 00 DAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 6 0 0
F E R TIL E0 .1 5 9 9 !
IN TERM ED IATE OTHEfl STRUCTURAL SPECIAL 0 .0 0 .0 0 0 9 7 0 .0 1 * 8 9 0 .0 0 0 2 7
UN S P EC IFIED0 .0 0 5 3 2
SUNS0 .3 0 7 3 7
CONV. R A TIO POWERtMNI 1 .0 8 7 8 8 9 .1 7 6 3 9 E 02
F IS S IL E !K G 1 8 .6 2 5 7 7 E 02
CORE A2 CORE A3
0 .1 2 3 1 50 .0 8 8 3 *
0 .1 * 7 0 90 .0 9 2 5 B
0 .0 0 .0 0 0 9 7 0 .0 0 .0 0 0 7 0
0 .0 1 3 2 6 0 .0 0 0 2 3 0 .0 0 8 3 2 0 .0 0 0 1 4
0 .0 0 * 7 30 .0 0 2 * 1
0 .2 8 9 * 30 .1 9 2 * 9
1 .0 1 0 3 80 .8 7 3 1 3
9 .0 3 * 8 9 E6 .* 3 9 6 9 E
020?
9 .6 6 8 9 3 E 02 1 .11073E 03
BLNK C l BLNK C2
0 .0 0 3 9 70 .0 0 3 0 6
0.0 * 3 5 1 0 .0 3 7 3 0
0 .0 0 .0 0 0 0 1 0 .0 0 .0 0 0 0 0
0 .0 0 3 7 * 0 .0 0 0 1 4 0 .0 0 3 1 1 0 .0 0 0 1 1
0 .0 0 0 1 20 .0 0 0 0 9
0 .0 5 1 * 90 .0 * 3 6 8
1 0 .5 8 * 6 11 1 .7 6 * 7 7
3 .2 8 6 7 5 E2 .6 6 1 9 * E
0101
7 .3 6 5 7 8 E 01 6 .9 2 * 9 IE 01
BLNK C3 BLNK B1
0.0 0 1 3 80 .0 0 2 8 0
0 .0 2 2 6 6 0 .0 * 0 9 8
0 .0 0 .0 0 0 0 0 0 .0 0 .0 0 0 0 0
0 .0 0 1 8 7 0 .0 0 0 0 6 0 .0 0 2 3 2 0 .0 0 0 0 *
0 .0 0 0 0 *0 .0 0 0 1 1
0 .0 2 6 0 30 .0 * 6 2 6
15.8 2 1 1 11 3 .9 3 6 6 8
1 .3 * 6 * 6 E2 .9 5 0 0 5 E
0101
5 .1 9 8 6 2 E 01 9 .0 5 2 0 0 E 01
BLNK B2 RFLTR E
0 .0 0 1 2 70 .0
0 .0 1 8 1 20 .0
0 .0 0 .0 0 0 0 0 0 .0 0 .0
0 .0 0 1 0 5 0 .0 0 0 0 2 0 .0 0 3 0 9 0 .0 0 0 0 *
0 .0 0 0 0 30 .0
0 .0 2 0 4 90 .0 0 3 1 *
1 3 .9 7 * * 00 .0
9 .7 8 2 7 9 E0 .0
00 9 .3 7 5 1 6 E 01 0 .0
ftFLTft 6 0 .0 0 .0 0 .0 0 .0 0 .0 0 5 8 3 0 .0 0 0 0 8 0 .0 OTHER LO S S ES ' BASED ON S T A R T-O F -S TE P TOTAL LOSSES
0 .0 0 5 9 10 .0 1 3 7 4
0*0 0 .0 0 .0
OVERALL 0 .3 * 9 9 7 0 .5 6 2 1 5 0 .0 0 .0 0 2 6 6 0 .0 5 7 * 9 0 .0 0 1 1 3 0 .0 1 2 8 6 1 .0 0 0 0 0 1 .4 1 5 1 5 2 .5 7 7 3 3 E 03 3 .3 1 9 3 6 E 03
POWER NORMALIZATION 01.99*3*, MAXIMUM POWER D E N S ITY * .6 6 1 3 * 3 E 02 IN ZONE 1 AT END SUBSTEP 1
AFTER STEP 1 OF CYCLE 3 , THE TIM E IS 7 5 .0 0 0 0 OAYS. THE TIM E STEP MAS 7 5 .0 0 0 0 D AYS, AND JO TA L TIM E IS 3 7 5 .0 0 0 0 DAYS
o oro
MULTI-CYCLE BREEDER (SHEARED RODS ADJUSTED, RECYCLE FEED DETERMINED)12XSX3 GROUPS, 288 P O IN TS I R - Z ) . STREAM OF C IT A T IO N CASES ORNL 72
SUMMARY OF NEUTRON LO S SES, E T C . FOR STEP 1 CYCLE 3 AT CYCLE DEPLETION T IN E 3 7 .5 0 D A YS. F IS S IL E KG IS AT 7 5 .0 0 OAYS
ZONE CLASS F IS S IL E F E R TIL E IN TERM EDIATE OTHER STRUCTURAL SPECIAL UN S P EC IFIED CORE A l 0 .1 2 6 3 2 0 .1 5 9 1 1 0 .0 0 .0 C 0 9 9 0 .0 1 4 8 9 0 .0 0 0 2 7 0 .0 0 6 0 4
SUMS0 .3 0 7 6 2
CONV. R A TIO POWER(PWI 1 .0 7 9 1 3 9 .1 9 2 2 6 E 02
F IS S IL E (K G ) 8 .6 7 7 9 0 E 02
CORE A2 CORE A3
0 .1 2 3 0 9 0 .1 4 6 4 6 0 .0 0 .0 0 0 9 8 0 .0 1 3 2 6 0 .0 0 0 2 3 0 .0 0 5 3 3 0 .0 8 8 0 3 0 .0 9 2 3 4 0 .0 0 .0 0 0 7 0 0 .0 0 8 3 2 0 .0 0 0 1 4 0 .0 0 2 6 7
0 .2 8 9 3 40 .1 9 2 2 0
1 .0 0 6 0 60 .8 7 3 6 4
9 .0 2 8 3 0 E6 .4 1 9 9 7 E
0202
9 . 66699E 1 .1 0 3 5 7 E
0203
BLNiC Cl BLNK C2
0 .0 0 4 5 4 0 .0 4 3 4 2 0*0 0 .0 0 0 0 1 0 .0 0 3 7 4 0*00014 0 .0 0 0 1 4 0 .0 0 3 4 6 0 .0 3 7 2 4 0 .0 0 .0 0 0 0 1 0 .0 0 3 1 1 0 .0 0 0 1 1 0 .0 0 0 1 1
0 .0 5 1 9 90 .0 4 4 0 4
9 .2 3 7 5 41 0 .3 6 4 8 6
3 .5 9 7 3 3 E2 .8 B 4 3 7 E
0101
9.5 1 9 4 7 E 8 . 79452E
01OJ
BLNK C3 BLNK B l
0 .0 0 1 5 4 0 .0 2 2 6 4 0 .0 0 .0 0 0 0 0 0 .0 0 1 B 7 0 .0 0 0 0 6 0 .0 0 0 0 5 0 .0 0 3 1 4 0 .0 4 0 9 3 0 . 0 0 .0 0 0 0 0 0 .0 0 2 3 2 0 .0 0 0 C 4 0 .0 0 0 1 2
0 .0 2 6 1 60 .0 4 6 5 5
1 4 .2 2 0 6 41 2 .4 3 4 4 3
1 .4 3 0 5 0 E3 .1 3 4 9 5 E
0101
6 .3 6 8 8 2 E1 .U 2 0 9 E
0102
BLNK B2 HFLTR E
0 .0 0 1 3 3 0 .6 1 8 1 1 0 .0 0 .0 0 0 0 0 0 .0 0 1 0 5 0 .0 0 0 0 2 0 .0 0 0 0 3 0 .0 0 .0 0 .0 0 .0 0 .0 0 3 0 9 0 .0 0 0 0 4 0 .0
0 .0 2 0 5 40 .0 0 3 1 4
1 3.283810 .0
1■01343 E 0 .0
01 1.0 3 1 9 2 E0 .0
02
H h .TR 0 6 .6 6 .6 6 .6 0 .0 0 .0 0 5 8 3 0 .0 0 0 0 8 0 .0OTHER LO S SES' BASED ON S T A R T -C F -S T E P TO TAL LOSSES
0 .0 0 5 9 10 .0 1 2 5 0
0 .0 0 .0 0 .0
mm M ~ w —OVERALL 0 .3 5 1 4 5 0 .5 6 0 2 5 0 .0 0 .0 0 2 6 9 0 .0 5 7 4 9 0 .0 0 1 1 3 0 .0 1 4 4 9 1 .0 0 0 0 0 1 .4 0 4 0 7 2 .5 8 4 6 6 E 03 3 .3 9 9 2 9 E 03
T IM E STEP THERMAL ENERGY, MW-HRS 4 .6 5 2 3 8 E 06 ANO TCTAL IS 2 .3 2 4 9 9 E 07
TIM E STEP 1. REQUIRED 0 .0 8 5 MINUTES CPU T IM E , AND 0 .6 6 4 MINUTES CLOCK TIM E
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIM E 7 5 .0 0 0 0 DAYS TO TA L T IN E 3 7 5 .0 0 0 P •>a y s
ITE R A TIO N FLUX CHANGE BETA MU-1 M U-2 MU-3 K SEARCH FACTORCROSS SECTIO NS UPDATED M ITH 1 .1 8 2 3 9 D -0 2
21CROSS SECTIONS UPDATED
3 .5 2 8 5 9 E -0 5 1 .3 9 1 7 4 -0 .8 0 2 1 3 -0 .7 4 7 6 1 1 .2 4 1 2 4 1 .0 0 0 0 0 4 2 .0 4 2 5 3 0 -0 5W ITH -3 .9 6 9 7 4 0 -0 4
CONVERGENCE IN D IC A TIO N BY M IN IM IZ IN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 1 .0000019 K 1 .0 0 0 0 0 4 8
END OF C R IT IC A L IT Y SEARCH - IT E R A T IO N TIM E 0 .0 3 9 HINUTES
IN PU T R E L A TIV E CONCENTRATION CHANGE TIM ES 1 .1 4 2 6 S E -0 2 HAS BEEN ADDED TO THE I N I T I A L SEARCH CONCENTRATIONS
FRACTIO N ABSORPTION IN SEARCH NUCLIDES 0 .0 0 4 9 4 ?
LEAKAGE 1.57705E 18 TOTAL LOSSES 1 .1 2 G 3 9 E 20 TO TA L PRODUCTIONS 1 .1 2 0 3 9 E 20 REACTOR PQhER (M ATTS) 2 .5 7 7 3 2 E 09
POKER NORMALIZATION 0 .9 4 4 S 8 , MAXIMUM POkEk D E N S IT Y 4 .7 1 5 0 2 2 6 02 IN ZONE 1 AT END SUBSTEP 1
AFTER STEP 2 OF CYCLE 3 , THE TIM E IS 1 5 0 .0 0 0 0 DAYS. THE TIM E STEP MAS 7 5 .0 0 0 0 OAYS, AND TO TAL TIM E IS 4 5 0 .0 0 0 0 DAYS*************>>***************** *4 ****fi* **************** ************ *******#*****************.*#%********************** *******
M U LTI-C Y C LE BREEDER (SHEARED RODS A D JU S TED . RECYCLE FEED DETERMINED)12X8X3 GROUPS. 288 PO IN TS I R - Z i . STREAM OF C IT A T IO N CASES ORNL 72
SUHFMftV OF NEUTRON LOSSES. E T C . FOR STEP 2 CYCLE 3 AT CYCLE DEPLETION TIM E 1 12.50 D AYS. F IS S IL E KG I S A T 1 5 0 .0 0 DAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 8 0 3
F E R TIL E0.1 5 8 9 2
IN TERM EDIATE OTHER STRUCTURAL SPECIAL 0 .0 0 .0 0 1 0 2 0 ,0 1 5 0 1 0 .0 0 0 2 8
UN S PEC IFIED0 .0 0 8 6 1
SUMS0 .3 1 1 8 7
CONV. R A TIO 1 .0 6 0 7 7
POWER1MM) 9 .3 2 4 7 2 c 02
F IS S IL E !K G ) 8 .7 1 7 4 1 E 02
CORE A2 CORE A3
0 .1 2 1 0 70.0 8 5 2 8
0 .1 4 2 9 90 .0 8 9 6 0
0 .0 0 .0 0 0 9 8 0 .0 0 .0 0 0 6 9
0 .0 1 3 0 50 .0 0 8 1 1
0 .0 0 0 2 30 .0 0 0 1 4
0 .00733 0 .0 0 3 6 7
0 .2 8 5 6 50 .1 8 7 5 0
0 .9 9 6 9 60 .8 7 4 5 4
8 .8 8 8 0 3 E 02 6 .2 2 6 4 0 E
9 . 65879E 1 . 09667E
02??
BLNK C l BLNK C2
0 .0 0 5 8 40 .0 0 4 2 9
0 .0 4 4 6 20 .0 3 7 3 5
OrO 0 .0 0 0 0 1 0 .0 0 .0 0 0 0 1
0 ,0 0 3 8 50 .0 0 3 1 3
0 .0 0 0 1 50 .0 0 0 1 1
0 .0 0 0 1 90 .0 0 0 1 4
0 .0 5 4 6 60 .0 4 5 0 2
7 .3 5 5 5 98 .3 8 3 7 5
4 .4 3 0 7 8 E 01 3 .3 9 7 2 4 E 01
1 .1 6 5 8 9E 1.0 6 1 9 1 E
0202
BLNK C3 OLNK 81
0 .0 0 1 8 20 .0 0 3 7 3
0 .0 2 2 4 40 .0 4 0 2 0
0 .0 0 .0 0 0 0 0 0 .0 0 .0 0 0 0 1
0 .0 0 1 8 60 .0 0 2 2 8
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 60 .0 0 0 1 4
0 .0 2 6 2 50 .0 4 6 3 9
1 1 .8 5 0 4 81 0 .2 6 0 7 3
1 .6 0 4 0 7 E3 .4 8 1 3 0 E
0101
7 .5 1 0 1 5 E 01 1 .3 1 1 2 8 E 02
BLNK B2 RFLTR E
0 .0 0 1 4 50 .0
0 .0 1 7 9 5 0 .0
0 .0 0 .0 0 0 0 0 0 .0 0 .0
0 ,0 0 1 0 40 .0 0 3 0 8
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 30 .0
0 .0 2 0 4 90 .0 0 3 1 3
1 2 .0 9 1 8 20 .0
1 .0 9 1 5 7 E0 .0
01 1 . 12463E 0 .0
02
RtU.TR D 0 .0 6 .0 0 .0 0 .0 0 .0 0 5 9 9 0 .0 0 0 0 8 0 .0 0 0 0 0 OTHER LO S SES' BASED ON S T A R T -O F -S TE P TO TAL LOSSES
0 .0 0 6 0 80 .0 1 2 9 8
0 .0 0 .0 0 .0
OVERALL 0 .3 5 1 5 2 0 .5 5 4 0 8 0 .0 0 .0 0 2 7 3 0 .0 5 7 4 1 0 .0 0 1 1 4 0 .0 2 0 1 5 1 .0 0 0 0 0 1 .3 8 6 6 4 2 .5 8 3 9 6 E 03 3 .4 7 5 7 6 E 03
T IH E STEP THERMAL ENERGY, HW-HRS 4 .6 5 1 1 3 E 06 AND TOTAL IS 2 .7 9 0 1 0 E 07
TIM E STEP 2 REQUIRED 0 .0 7 2 M INUTES CPU T IM E . AND 0 .6 3 7 MINUTES CLOCK TIM E
A FIN A L FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 TO TA L D EP LETIO N TIM E 4 5 0 .0 0 0 DAYS i t e r a t i c JN F l u x CHAnGF BETC m u- 1 R iF 5 H1P1 k s e a r c h f a c t o r
____________________________________________________________________________________________ CROSS SEC TIO N S UPDATED W ITH 1 .0 1 2 8 0 0 -0 2CROSS SECTIONS UPDATED W ITH -3 .5 6 8 6 3 D -0 4
21 3 .1 4 7 1 3 E -0 5 1 .3 9 1 7 4 -0 .B 1 7 3 1 -0 .7 7 7 1 9 1 .2 9 1 7 8________ 1 .0 0 0 0 0 4 1 .8 7 2 7 4 0 -0 5 _______________________
CONVERGENCE IN D IC A TIO N BY M IN IM IZIN G THE SUM OF THE SQUARES OF THE RESIOUES - R E L A TIV E ABSORPTION 1 .0 0 0 0 0 1 0 K 1 .0 0 0 0 0 4 8
fcrt'j OF C R IT 1 C A L IT Y SEARCH - IT E R A T IO N TIM E 0 .0 4 2 MINUTES _____
I NPUT R ELATIV E CONCENTRATION CHANGE TIM ES 9 .7 7 1 0 9 E -0 3 HAS BEEN ADDED TO THE IN IT I A L SEARCH CONCENTRATIONS
FR ACTIO N ABSORPTION IN S'-ARCH NUCLIDES 0 .0 0 7 0 8 8 _______________________________________________________________________________________________
LEAKAGE 1 .6 1 5 9 9 E 18 TOTAL LOSSES l r l ? - ' 20 TO TA L PRODUCTIONS 1 .1 2 0 6 2 E 20 REACTOR POWER!MATTS) 2 .5 7 7 3 2 E 09
MULT I —CYCLE BREEDER I SHEARED ROCS A D JU S TED , RECYCLE FEED DETERM INED)12X8X3 GROUPS. 288 PO IN TS ( R - Z ) . STREAM OF C IT A T IO N CASES ORNL 72
FIN A L SUNNARY OF NEUTRON LOSSES* E T C . FOR CYCLE 3 TOTAL D EPLETION TIM E 4 5 0 .0 0 DAYS
ZONE CLASS CORE
F IS S IL EO .L 2 9 I7
F E R TIL E0 .15921
IN TERM EDIATE0 .0
OTHER STRUCTURAL 0 .0 0 1 0 4 0 .0 1 5 1 0
S P ECIA L0 .0 0 0 2 B
U N S PEC IFIED0 .0 1 0 3 1
SUMS0 .3 1 5 1 2
CONV. R A TIO 1 .0 5 1 3 8
PQHER(HH) 9 .4 2 1 2 2 E 02
F IS S IL E (K G ) 8 . 7174 IE 02
CORE A2 CORE A3
0 .1 1 9 2 90 .0 8 3 1 3
0 .1 4 0 3 90 .0 8 7 4 0
0 .00 .0
0 .0 0 0 9 80 .0 0 0 6 8
0 .0 1 2 8 60 .0 0 7 9 3
0 .0 0 0 2 20 .0 0 0 1 4
0.0 0 B 550 .0 0 4 3 0
0 .2 8 2 2 80 .1 8 3 5 7
0 .9 9 2 3 10 .8 7 4 9 6
S .7 6 5 2 4 E6 .0 7 2 7 2 E
0202
9 .6 5 8 7 9 E1.0 9 6 6 7 E
0203
BLNK C l BLNK C2
O.ODAAO0.0 0 4 7 1
0 .0 4 5 8 /0 .0 3 7 5 6
0 .00 .0
6.OOO010 .0 0 0 0 1
0 .6 0 3 9 60 .0 0 3 1 5
0 .0 0 0 1 50 .0 0 0 1 1
0 .0 0 0 2 20 .0 0 0 1 5
0 .0 5 6 8 10 .0 4 5 6 8
6 .6 7 1 4 97 .6 5 7 0 0
4 .9 7 2 6 2 E3 .6 9 2 9 0 E
0101
1 .16569E1 .0 6 1 9 1 E
0202
BJLNK C3 BLNK B1
0 .0 0 1 9 60 .0 0 3 9 9
0 .0 2 2 3 2 0 .0 3 9 6 3
0 .00 .0
0 .0 0 0 0 00 .0 0 0 0 1
0.001.850 .0 0 2 2 5
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 60 .0 0 0 1 5
0 .0 2 6 2 50 .0 4 6 0 5
1 0 .9 4 9 2 29 .4 5 0 1 9
1 .6 9 5 4 5 £ 3 .6 4 4 5 0 E
0101
7.5 1 0 1 5 E1.31128E
0102
BLNK B2 RFLTR E
0 .0 0 1 5 00 .0
0 .0 1 7 8 40 .0
0 .00 .0
o .o o o c o0 .0
0 .0 0 1 0 30 .0 0 3 C 8
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 40 .0
0 .0 2 0 4 30 .0 0 3 1 2
1 1 .5 7 3 9 70 .0
1 .1 3 5 7 0 E0 .0
01 1. 12463E 0 .0
02
RFLTll fl 0 .0 d .6 0 .0OTHER LOSSES
0 .0 0 .0 0 6 1 6 0 .0 U 0 0 8 0 .0 0 0 0 0 • BASED ON S T A R T -O F -S TE P TOTAL LOSSES
0 .0 0 6 2 40 .0 1 4 4 3
0 .0 0 .0 0 .0
OVERALL 0 .3 5 0 3 5 0 .55021 0 .0 0 .0 0 2 7 3 0 .0 5 7 3 7 0 .0 0 1 1 4 0 .0 2 3 7 7 I . 00000 1 .3 8 0 3 1 2 .5 7 7 3 3 E 03 3 .4 7 5 7 6 E 03
REPEAT CYCLE CONVERGENCE IS 4 .3 7 3 8 2 E — 02
RFPFA TIN G CYCLE 3 ITE R A TIO N NUMBER 3
___________________________________ M U LTI-C Y C LE BREEDER (SMEARED RODS AD JUSTED , RECYCLE FEED DETERM INED)12X8X3 GROUPS, 288 P O IN TS (R ~ Z I . STREAM OF C IT A T IO N CASES ORNL 72
STAftf" FUEL WWSgBEBT PMTVCCE----- 2--------------------------------------------------------------------------------------------------------------------
Che f a c t o r A p p lie d To th e r e c y c le f r a c t i o n f o r re p e a t c y c le is s .8 0 3 1 7 e -o i
END F^UEL MANAGEMENT FOR CYCLE T
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIM E 575 DAYS TO TAL TIM E 3 0 0 .0 0 0 0 DAYS
M U LTI-C Y C LE BREEDER (SHEARED RODS A D JU S TED . RECYCLE FEED DETERMINED)________________________________________________12X8X3 GROUPS. 288 PO INTS ( R - Z ) . STREAM OF C IT A TIO N CASES ORNL 72
L IN E RELAXATION H IL L BE DONE ON ROWS AND COLUMNS - 1 INNER IT E R A T IO N (S )_____________________________________________________________________L IM IT IN G VALUES OF THE SEARCH FACTOR FOR ABSORPTION AND TO TA L LOSS ARE -2 .4 3 1 3 4 E 00 -4 .8 8 9 3 9 E 00ITE R A TIO N FLUX CHANGE BETA________ H U -1________ H U -2 ________ MU-3________________ K SEARCH FACTOR____________________________________________
CROSS SECTIONS UPDATED WITH -5 .7 4 1 0 1 0 -0 2___________________________________________________________________________________________ CROSS SECTIONS UPDATED W ITH 1 .7 8 7 3 8 0 -0 3 _______________________
23 - 1 . 5 t i 0 5 E - 0 4 1 .3 9 1 7 4 -1 .9 0 3 5 0 -1 .5 9 4 6 5 2 .6 7 0 7 6 0 .9 9 9 9 8 4 -7 .0 7 4 J 7 0 -0 5
CONVERGENCE IN D IC A TIO N BY M IN IM IZIN G THE SUM OF THE SQUARES OF THE RESIDUES - R E L A TIV E ABSORPTION 0 .9 9 9 9 9 2 9 K 0 .9 9 9 9 8 9 9
END 0 7 " C R IT IC A L IT Y SEARCH - ITE R A TIO N TIM E 0 .0 4 6 MINUTES 1
IN P U f R E L A TIV E CONCENTRATION CHANGE TIM ES -5 .5 6 2 2 7 E -0 2 HAS BEEN ADDED TO THE I N I T I A L SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 0 2 5 0 1
LEAKAGE 1.54O02E 18 rOTAL LbSSES 1 .1 2 0 1 3 E 20 TOTAL PRODUCTIONS F .1 2 0 1 3 E 20 REACTOR POWER!MATTS) 2 .5 7 7 2 ’ E 09
M U LTI-C Y C LE BREEDER (SHEARED RODS A D JUS TED , RECYCLE FEED O ETERH IN EO )12X8X3 GROUPS, 288 PO IN TS ( R - Z I . STREAM OF C IT A T IO N CASES ORNL 72
SUrtHAfcY OF NEUTRON LOSSES'i E T C . BEFORE D EP LETIN G STEP 1 OF CYCLE 3 TO TA L D EP LETIO N TIM E 3 0 0 . 00 DAYS
ZONE CLASS CORE A1
F IS S IL E0 .1 2 5 9 9
F E R TIL E0 .1 5 9 8 7
INTERM EDIATE OTHER STRUCTURAL 0 . 0 9 .0 0 0 9 7 0 .0 1 4 8 9
SPECIAL0 .0 0 0 2 7
U N SP EC IFIED0 .0 0 5 3 7
SUMS0 .3 0 7 3 6
CONV. R A T IO P O H E M M il 1 .0 8 7 6 8 9 .1 7 5 B 8 E 02
F I S S l L E t K G i 8 .6 2 7 1 IE 02
C o r e A2CORE A3
0*12315 0 .0 8 8 3 5
0 .1 4 7 0 70 .0 9 2 5 7
O .D 0 .0 0 0 9 7 0 .0 0 .0 0 0 7 0
0 .0 1 3 2 60 .0 0 8 3 1
0 .0 0 0 2 30 .0 0 0 1 4
0 .0 0 4 7 7 0 .00243
0 .2 6 9 4 40 .1 9 2 5 0
1 .0 1 0 2 00 .8 7 2 9 7
9 .0 3 5 0 S E 6 . 4 4010E
0292
9 .6 7 0 4 6 E 02 1 .1 1 0 9 IE 03
s l n k . c iBLNK C2
0 .0 0 3 9 70 .0 0 3 0 6
0 .0 4 3 5 00 .0 3 7 3 0
0 .0 0 .0 0 0 0 1 0 .0 0 .0 0 0 0 0
0 .0 0 3 7 40 .0 0 3 1 1
0 .0 0 0 1 40 .0 0 0 1 1
0 .0 0 0 1 20 .0 0 0 0 9
0 .0 5 1 4 80 .0 4 3 6 7
1 0 .5 8 4 5 91 1 .7 6 4 7 4
3 .2 8 6 2 1 E 2 .6 6 1 6 7 6
01Q1
7.3 6 5 7 8 E 6.92491C
0101
BLNK C3 BLNK B l
0 .0 0 1 3 80 .0 0 2 8 0
0 .0 2 2 6 60 .0 4 0 9 8
0 .0 0 .0 0 0 0 0 0 .0 0 .0 0 0 0 0
0 .0 0 1 8 70 .0 0 2 3 2
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 40 .0 0 0 1 1
0 .0 2 6 0 20 .0 4 6 2 5
1 5 .8 2 1 0 613.93661
1 .3 4 6 3 8 E 2 .9 4 9 9 2 E
01P I
5 . 19862E 9 . 05200E
0101
BLNK B2 RFt.TR E
0 .0 0 1 2 70 .0
0 .0 1 8 1 20 .0
0 .0 0 .0 0 0 0 0 0 .0 0 .0
0 .0 0 1 0 50 .0 0 3 0 9
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 30 .0
0 .0 2 0 4 90 .0 0 3 1 4
1 3 .9 7 4 3 80 .0
9 .7 8 2 3 3 E0 .0
0!) 9 .3 7 5 1 6E 0 .0
01
6 N .tR 0 0 .0 0 .0 0 .0 0 .0 0 .0 0 5 8 3 0 .0 0 0 0 8 0 .0 OTHER LOSSES* BASED ON S TA R T -O F -S TE P TO TAL LOSSES
0 .0 0 5 9 10 .0 1 3 7 3
0 .0 0 .0 0 .0
OVERALL 0 .3 4 9 9 6 0 .5 6 2 0 7 0 .0 0 .0 0 2 6 6 0 .0 5 7 4 8 0 .0 0 1 1 3 0 .0 1 2 9 7 1 .0 0 0 0 0 1.4 1 4 9 3 2 .5 7 7 3 3 E 03 3 .3 1 9 3 3 6 03
POWER NORMALIZATION 0 .9 9 4 3 5 , MAXIMUM POWER D E N S ITY 4 .6 6 1 0 3 8 6 02 IN ZONE 1 AT END SUBSTEP 1
AFTER STEP I OF CYCLE 3 , THE TIM E I S 7 5 .0 0 0 0 OAVS. THE T IH E STEP WAS 7 5 .0 0 0 0 OAVS, ANO TOTAL TIM E IS 3 7 5 .0 0 0 0 DAYS********************************t«************************»***«******************* **************************** *************** 288
H U lT l -C Y C ie BREEDER (SHEARED BODS ADJUSTED. RECYCLE f E E r OETERH IN ED >12X8X3 CROUPS. 268 POINTS I R - Z ) . STREAM OF C ITATION CASES . RNL 72
SUMMARY OF NEUTRON LOSSES, ETC. FOR STEP 1 CYCLE 3 AT CYCLE DEPLETION TIME 3 7.50 OAYS. F I55ILC K6 IS AT 75.00 OAYS
ZONE CLASS FISSILE FERTILE INTERMEDIATE CTHER :STRUCTURAL SPECIAL UNSPECIFIED SUMS CONV. RATIO POUEfttrUf F I S S I L E I K G )CORE A1 0.12631 0.15908 0 .0 0.00099 0.01489 0.00027 0.00608 0.30762 1.07895 9.19169E 02 8. 6791 IE 02CORE A2 0.12309 0.14643 0 .0 0.00096 0.01326 0.00023 0.00537 0r28936 1.00568 9»028<it£ 02 9.66840£ 02CORE A3 0.08804 0.0923 3 0 .0 0.00070 0.00831 0.0CS14 0.00273 b . 19222 0.87348 6 .42037E 02 1.10374E 03BLNK Cl 0.00454 0. 04341 0 .0 0.00001 0.00374 0.00014 0.00014 0.05198 9.23774 3.59667b 01 9 .51907E 01BLNK C2 0.00346 0.03724 0.0 0.00001 0.00311 0.00011 0.00011 0.04403 10.36498 2.8S405E 01 6 .79429E 0*BLNK. C3 0.00154 0. 02264 0 .0 0.0 0 0 0 0 ' 0.001C7 O.C0006 0.00005 0.02616 14.22073 1.43041E 01 6.3687 IE 01BLNK BI 0.00314 0.04093 0 .0 0 .000CO 0.00232 0.00004 0.00012 0.04655 12.43449 3.13479E 01 1.1120SE 02BLftK B2 0.00133 0.01811 0 .0 0.00000 0.00105 0.00002 0.00003 0.02054 13.283 83 1 «0'.338E 01 1.0319IE 02RFLTR E 0 .0 0 .0 0 .0 0 .0 0.00309 0.00004 0 .0 0.00314 0 .0 0 .0 0 .0RFLTfT 5 0.0 6 .0 ti.Ti O .c 0.00583 0.00008 0.0 0.00591 0 .0 0 .0 0 .0
OTHER LOSSES • BASED ON S T A R T -O F -S T E P TOTAL LOSSES 0 .Q125C
OVERALL 0.35144 0. 56017 0 .0 0.00269 0.05748 0.00113 0.01459 1.00000 1.40386 2.58464E 03 3.39971E 03
TIM E STEP THERMAL ENERGY. HW-HRS 4 .6 5 2 3 6 2 06 AND TOTAL IS 2 .3 2 4 9 9 E 07
TIM E STEP 1 RFQUIRED 0 .0 7 7 M INUTES CPU T IM E , AND 0 .6 55 M INUTES CLOCK TIM E__________________________________
A FLUX - EIGENVALUE PROBLEM FOLLOWS FOR CYCLE 3 CYCLE TIM E 7 5 .0 0 0 0 OAYS___ TOTAL T IM E ____3 7 5 .0 0 0 0 OAYS
I t e r a t i o n ~ f lu x t h a n ^ I b it s m u -i m u-2 h u -3 k s e a rc h f a c t o r '___________________________________________________ ________________________ CROSS SECTIONS UPDATED W ITH 1.173150-02___________________________ rO
' ' " ' CROSS SECTIO N S UPDATED W ITil -3 .9 6 rtB 5 D -0 4 CO21________ 3 .5 2 8 5 9 E -0 5 1 .3 9 1 7 4 -0 .8 0 5 4 1 -0 .7 9 3 2 9 , i ‘«'.86________ 1 .0 0 0 0 0 4 1 .9 8 1 7 6 0 -0 5 _________________________________________________ \ Q
CONVERGENCE INDtC AT IO N BY H IN 1 M U IN G THE SUM OF THE S Q ^ r .E S OF THE RESIDUES - R E LA TIV E ABS0PPT1QN 1 .0 0 0 0 0 1 0 ___K 1 .0 0 0 0 0 4 6
END OF CR1T1CAL1TY SEARCH - I T E R M ! OS T IM C 0 .0 4 6 H1NUT1 ?___________________________________________________________________________________________
INPUT R ELA TIV E CONCENTRATION CHANGE TIM ES 1 .1 3 8 5 5 E -0 2 HAS ~EN ADDED TO THE IN IT IA L SEARCH CONCENTRATIONS______________________
FRACTION ABSORP TIO N IN SEARCH NUCLtOES 0.0050*.2______________________________________________________________________________________________________
_____LEAKAGE 1.57694E IB TOTAL LOSSES 1 .1 2 0 3 9 E 20 TOTAL PRODUCTIONS 1 .1 2 0 3 9 E 20 REACTOR POWSRtWATTS) 2._57 7 3 2 E _ 0 * = _ _
-POUCT-Ti£lKJrei.TZmi)N A .M 4 S 9 , -ffiUrRijfTPOWEfi DENSITY 4.714592E 02 IN ZONE 1 AT END SUBSTEP 1
AFTER STEP 2 OF CYCLE 3 . THE TIME 7S 150.0000 DAYS. THE TIME STEP MAS 75.0000 DAYS. AND TOTAL TIME IS 450.0000 OAYS
M U LTI-C Y C LE 8REE0ER ( SHEARED RODS A D JU S TED . RECYCLE FEED OETERM INEOI'1 2 X 8 X 3 GROUPS, 288 P O IN IS ( R - 2 I . STREAM OF C IT A T IO N CASES ORNL 72
~ “ 5UHMIIW“ OF TICOTftM LTJ55R;■■ETC": HHC STEf>~2 CyClT T ~aT CV tLE bEP LETIO N TIM E 1 1 2 .5 0 DAYS. F IS S IL E KS IS AT 1 5 0 .0 0 OAYS
ZONE tLASS CORE A1
F IS S IL E0 .1 2 8 0 2
F E R TIL E INTERM EDIATE 0 .1 5 8 8 9 0 .0
OTHER0 .0 0 1 0 2
STRUCTURAL0 .0 1 5 0 0
SPECIAL0 .0 0 0 2 8
U N S P EC IFIED0 .0 0 8 6 5
SUNS0 .3 1 1 8 5
CCNV. R A TIO 1 .06061
PQMER(MN) 9 .3 2 3 9 3 E 02
F I S S IL E I KG) 8 .7 1 8 4 9 E 02
CORE A2 CORE A3
0 .lfe l6 70 .0 8 5 2 9
0 . 14298 0 .0 8 9 5 9
0 . 00 .0
0 .0 0 0 9 80 .0 0 0 6 9
0 .0 1 3 0 50 .0 0 8 1 1
0 .0 0 0 2 30 .0 0 0 1 4
0 .0 0 7 3 60 .0 0 3 6 9
0 .2 8 5 6 60 .1 8 7 5 2
0 .9 9 6 8 00 .8 7 4 3 9
8 .8 8 8 2 5 c6 .2 2 6 9 6 E
0202
9 . 66007E 1 .0 9 6 8 4 E
020 ?
BIN* Cl BLNK C2 0*00429
0.0 4 4 6 1 0 .03735.
6 . 00 . 0
0 .6 0 0 0 10 .0 0 0 0 1
0 .0 0 3 8 50 .0 0 3 1 3
0 .0 0 0 1 50 .0 0 0 1 1
0*000190 .0 0 0 1 4
0 .0 3 4 6 50 .0 4 5 0 1
7 .3 5 6 0 08 .3 8 4 0 1
4 .4 2 9 7 8 E3 .3 9 6 8 7 E
0101
I . 1653IE 1 .06186E
0292
BLNK C3 BLNK B1
0*001820 .0 0 3 7 3
0 . 02244 0 .0 4 0 2 0
0 . 00 . 0
0 .0 0 0 0 0O .O O uO l
0 .0 0 1 8 60 .0 0 2 2 8
0 .0 0 0 0 60 .0 0 0 0 4
0 .0 0 0 0 60 .0 0 0 1 4
0 .0 2 6 2 40 .0 4 6 3 9
1 1 .8 5 0 7 01 0 .2 6 0 8 7
1 .6 0 3 9 9 E3 .4 8 1 2 2 E
0101
7 .5 0 9 9 7 E1.3 1 1 2 6 E
0102
BLNK B2 RFLTR E
0 .0 0 1 4 50 . 0
0 .6 1 7 $ *0 .0
0 . 00 . 0
O.OOOGQ0 .0
0 .0 0 1 0 40 .0 0 3 0 3
0 .0 0 0 0 20 .0 0 0 0 4
0 .0 0 0 0 30 . 0
0 .0 2 0 4 90 0 0 3 1 3
1 2 .0 9 1 8 80 . 0
1 .0 9 1 5 5 E0 . 0
01 1 . 12462£0 . 0
02
R U T * 0 0 . 0 6 . 0 6 . 0OTHER LOSSES'
0 .0 0 .0 0 5 9 9 0 .0 0 0 0 8 0 .0 BASED CN S T A R T -O F -S T E P TO TA L LOSSES
0 .0 0 6 0 80 .0 1 2 9 8
0 . 0 0 . 0 0 . 0
OVERALL 0.3 5 1 5 1 0 .5 5 4 0 0 0 . 0 0 .0 0 2 7 3 0 .0 5 740 0 .0 0 1 1 4 0 .0 2 0 2 5 1.0 0 0 0 0 1 .3 8 6 4 6 2 .5 8 3 v ^ E 03 3 .4 7 6 1 5 E 03
T IM E STEP tHERMAL ENERGY, MW-HRS 4 .6 5 1 H E 06 ANO TOTAL IS 2 .7 9 0 1 0 E 07
TIM E STEP 2 REQUIRED 0 .0 7 7 M INUTES CPU T IM E , »N0 0 .6 4 1 MINUTES CLOCK TIM E
A FIN A L FLUX - EIGENVALUE PROBLEM FOLLOWS FOR C-YCLE 3 TO TA L D EP LETION TIM E 4 5 0 .0 0 0 DAYSITE R A TIO N - 'F C U X CHANGE BETA M u -i mu- 2 M U-3 K SEARCH FACTOR
CROSS SECTIONS UPDATED W ITH 1 .0 0 B 3 3 D -0 2CROSS SECTIONS UPOATED WITH -3 .5 2 6 6 6 0 -0 4
21 3 .0 5 1 7 6 E -0 5 1 .3 9 1 7 4 -0 .7 6 1 8 7 -0 .6 9 8 3 8 1 .1 6 2 4 8 1 .0 0 0 0 0 4 1 .7 6 8 0 8 0 -0 5
CONVERGENCE IN D IC A TIO N BY M IN IM IZIN G THE SUM OF THE SQUARES OF THE RESIDUES - R E LA TIV E ABSORPTION 1 .0000010 K 1 .0 0 0 0 0 4 8
END OF C R ITIC A L I T Y SEARCH - ITE R A TIO N TIM E 0 .0 4 1 MINUTES
INPUT R E LA TIV E CONCENTRATION CHANGE T IK E S 9 .7 3 0 6 6 E -0 3 HAS BEEN AOOEO TO THE I N IT IA L SEARCH CONCENTRATIONS
FRACTION ABSORPTION IN SEARCH NUCLIDES 0 .0 0 7 1 7 3
LEAKAGE 1 .615906 18 TOTAL LOSSES 1 .1 2 0 6 3 E 20 TO TA L PRODUCTIONS 1 .1 2 0 6 3 E 20 REACTOR P0W ER{W ATTS) 2 .5 7 7 3 2 E 09
29
0
H U L TI-C V C L E BREEDER (SMEARED ROCS A C JU S TED , RECYCLE FEED DETERM INED)12X8X3 GROUPS, 288 PO IN TS ( R - Z ) . STREAK OF C IT A T IO N CASES ORNL 72
FIN A L SUMMARY OF NEUTRON LOSSES* E T C . FOR CYCLE 3 TO TAL 0EPLET10N TIM E 4 5 0 .0 0 DAYS
ZONE CLASS F IS S IL E F E R TIL E INTERM EDIATE OTHER STRUCTURAL SP ECIA L U N S PEC IFIED SUMS CONV. R A TIO POUERiMU) F IS S IL E IK G ICORE A1 0 .12916 0 .1 5 9 1 8 0 .0 0 .0 0 1 0 4 0 .0 1 5 0 9 0 .0 0 0 2 8 0 .0 1 0 3 5 0 .3 1 5 1 0 1 .0 5 1 2 4 9 .4 2 0 3 3 E 02 8 .71849E 02CORE A2 0 .1 1 9 2 9 0 .1 4 0 3 7 0 .0 0 .0 0 0 9 8 0 .0 1 2 8 6 0 .0 0 0 2 2 0 .0 0 8 5 8 0 .2 8 2 3 0 0 .9 9 2 1 7 8 .7 6 5 5 6 E 02 9 .6 6 0 0 7 E 02CORE A3 0 .0 8 3 1 4 0 .0 8 7 3 9 0 .0 0 .0 0 0 6 8 0 .0 0 7 9 3 0 .0 0 0 1 4 0 .0 0 4 3 2 0 .1 8 3 6 0 0 .8 7 4 8 1 6 .0 7 3 4 3 E 02 1 .09684E 03BLn k C l 0 .0 0 6 6 0 6 .0 * 5 6 6 576 0 .0 0 0 0 1 0 .0 0 3 9 6 0 .0 0 0 1 5 0 .0 0 0 2 2 0 .0 5 6 8 0 6 .6 7 1 9 5 4 .9 7 1 4 1 E 01 1 .165B 1E 02BLNK C2 0 .00471 0 .0 3 7 5 6 0 .0 0 .0 0 0 0 1 0 .0 0 3 1 4 0 .0 0 0 1 1 0 .0 0 0 1 5 0 .0 4 5 6 8 7 .6 5 7 2 9 3 .6 9 2 5 1 E 01 1 .0 6 1 8 6 E 02BLNK t 3 0 .0 0 1 9 6 0 .0 2 2 3 2 0 .0 0 .0 0 0 0 0 0 .0 0 1 8 5 0 .0 0 0 0 6 0 .0 0 0 0 6 0 .0 2 6 2 5 10.94945 1 .6 9 5 4 0 E 01 7 .5 0 9 9 7E 01BLNK B l 0 .0 0 3 9 9 0 .0 3 9 6 3 0 .0 0 .0 0 0 0 1 0 .0 0 2 2 5 0 .0 0 0 0 4 0 .0 0 0 1 5 0 .0 4 6 0 5 9 .4 5 0 3 4 3 .6 4 4 5 1 E 01 1 .31126E 02BLNK B2 0 .0 0 1 5 0 0 .0 1 7 8 4 0 .0 0 .0 0 0 0 0 0 .0 0 1 0 3 0 .0 0 0 0 2 0 .0 0 0 0 4 0 .0 2 0 4 3 11.5 7 4 0 3 1 .1 3 5 7 9 E 01 1 .1 2 4 6 2 E 02RFLTR E 0 .0 0 .0 0 .0 0 .0 0 .0 0 3 0 8 0 .0 0 0 0 4 0 .0 0 .0 0 3 1 2 0 .0 o .a 0 .0RFLTR D 0 .0 0 .0 6 .0 0 .0 0 .0 0 6 1 6 0 .0 0 0 0 8 0 .0 0 .0 0 6 2 4 0 .0 0 .0 C .O
OTHER LOSSES* BASED ON S T A R T-Q F -S TE P TO TA L LOSSES 0 .0 1 4 4 2
OVERALL 0 .3 5 0 3 5 0 .5 5 0 1 4 0 .0 0 .0 0 2 7 3 0 .0 5 736 0 .0 0 1 1 4 0 .0 2 3 8 5 1.0 0 0 0 0 1 .3 8 0 1 4 2 .5 7 7 3 3 E 03 3 .4 7 6 1 5 E 03
REPEAT CYCLE CONVERGENCE IS -3 .7 5 0 8 9 E -0 4
M U LTI-C Y C LE BREEDER (SHEARED RODS AD JUS TED , RECYCLE FEED DETERM INED! 12X8X3 GROUPS, 288 PO IN TS ( R - Z ) . STREAM OP C IT A T IO N CASES ORNL 72
START FUEL mitt'SEMENT'FMTVCEE-----J
ACCOUNTING INFORMATION (MASSES IN KG) FOLLOWS FOR CYCLE 1
FRESH FUEL FEED STREAM__ 1I N I T I A L INVENTORY 10 1 .0 2 6 4 8 E 01
16 2 .9 5 5 7 6 E 01 17 1 .1 8 2 8 2 E 0111 0 .0 12 3 .4 1 1 1 7 E 03 14 3 .9 6 0 8 6 E 02 15 1 .5 3 7 2 3 E 02
FRESH FUEL FEED STREAM 2I N I T I A L INVENTORY 10 1 .0 7 3 3 7 E 01
16 3 .3 7 2 5 6 E 01 17 1 .3 4 9 6 6 E 0111 0 .0 12 3 .5 6 7 14E 03 14 4 .5 2 1 8 0 E 02 15 1 .7 5 4 1 2 E 02
FRESH FUEL FEED STREAM 3I N I T IA L INVENTORY 10 1 .0 5 8 0 5 E 61
16 3 .9 4 6 9 7 E 01 17 1 .5 7 9 2 8 E 01l l 0 .0 12 3 .5 1 6 3 2 E 03 14 5 .2 8 9 2 2 E 02 15 2 .0 5 3 0 3 E 02
FRESH FUEL FEED STREAM 4I N I T I A L INVENTORY 10 1 .0 4 2 7 4 E 01
16 0 .0 17 0 .011 0 .0 12 3 .4 6 5 3 5 E 03 14 0 .0 15 0 .0
FRESH FUEL FEED STREAM 5I N I T I A L INVENTORY 10 1 .1 0 5 0 4 E O l
16 0 .0 17 0 .011 0 .0 12 3 .6 7 2 5 0 E 03 14 0 .0 15 0 .0
DISCHARGE STREAM 1LOADING 10 9 .5 2 4 6 4 E 01
16 9 .6 3 4 8 7 E 01 17 4 .2 1 5 5 9 E 0111 1 .5 6 8 0 6 E 00 12 3 .3 5 7 7 2 E 04 14 1.4 6 9 4 7 E 03 15 5 .4 8 8 3 4 E 02
DISCHARGES 10 1 .9 2 5 6 1 E 01 16 2 .4 0 8 7 0 E 01 17 1 .0 5 3 9 0 E 01
11 3 .5 3 5 7 0 E —01 12 6 .8 3 5 9 7 E 03 14 3 .6 1 7 6 8 E 02 15 1 .3 7 1 8 0 E 02
FRESH FUEL FEED STREAM 1FRESH FEEO 10 2 .0 7 7 5 3 E 01
16 2 .5 6 8 8 2 E 01 17 1 .0 2 7 9 4 E 0111 0 .0 12 6 .9 0 4 2 7 E 03 14 3 .4 4 2 9 7 E 02 15 1 .3 3 6 0 9 E 02
FRESH FUEL FEED STRFAM 2FRESH FEED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
FRESH FUEL FEED STREAM 3FRESH FEED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
FRESH FUEL FEED STREAM 4FRESH FEED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
FRESH FUEL FEED STREAM 5FRESH FEED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
MAKEUP STREAM 1RECYCLE FEED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
ro tA L NET FEEO 10 2 .5 6 6 2 U E 00 16 7 .3 8 9 4 2 E 00 17 2 .9 5 7 0 5 E 00
11 0 .0 12 8 .5 2 7 9 3 E 02 14 9 .9 0 2 1 5 E 01 15 3 .8 4 3 0 8 E 01
MAKEUP STREAM 2RECYCLE F-EED 10 0 .0
16 0 .0 17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
TOTAL n£T FEED 13 2 .6 8 3 4 2 E 00 16 8 .4 3 1 4 1 E 00 17 3 .3 7 4 1 5 E 00
11 0 .0 12 8 .9 1 7 8 3 E 02 14 1 .1 3 0 4 5 E 02 15 4 .3 8 5 2 9 E 01
MAKEUP STREAM 3RECYCLE FEED
16 0 .010 0 .0
17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
TOTAL NET FEED 16 9 .8 6 7 4 3 E 00
10 2 .6 4 5 1 2 E 0 0 17 3 .9 4 8 1 9 E 00
11 0 .0 12 8 .7 9 0 8 0 E 02 14 1 .3 2 2 3 1 E 02 15 5 .1 3 2 5 8 E 01
MAKEUP STREAM 4R E tY C LE F e e d
16 0 .010 <T."0
17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
TOTAL NET FEED 16 0 .0
10 2 .6 0 6 8 5 E 00 17 0 .0
11 0 .0 12 8 .6 6 3 3 8 E 02 14 0 .0 15 C .O
MAKEUP STREAM 5RECYCLE FEED
16 0 .010 0 .0
17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
TOTAL NET FEED 16 0 .0
10 2 .t 6 2 6 lE (TO 17 0 .0
11 0 .0 12 9 .1 8 1 2 5 E 02 14 0 .0 15 0 .0
MAKEUP STREAM 6r e c y Cl S ^ e e d
16 0 .010 0 .0
17 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
T O T A l N E T - *=eeb 16 0 .0
lO 2 .8 0 4 0 0 E 00 17 0 .0
I t 0 .0 12 9 .3 1 8 6 5 E 02 >4 0 .0 15 0 , 0
MAKEUP STREAM 7RECYCLE FEED
16 O .Q10 0 .0
I T 0 .011 0 .0 12 0 .0 14 0 .0 15 0 .0
VotAL NET <=EED 16 0 .0
10 4 . T o? oY e 00 17 0 .0
11 0 .0 12 .1.56429E 03 14 0 .0 15 0 .0
**********TO TALS SUMMED OVER STREAMS
LOADING 10 9 .5 2 4 6 4 E 01 11 1 .5 6 8 0 6 E 00 12 3 .3 5 7 7 2 E 04 14 1 .4 6 9 4 7 E 03 15 5 .4 8 B 3 4 E 0216 9 .6 3 4 8 7 E
DISCHARGES01 I T 4 .2 l5 $ 4 £ 01
10 1 .9 2 5 6 1 E 01 11 3 .5 3 5 7 0 E — 01 12 6 .8 3 5 9 7 E 03 14 3 .6 1 7 6 8 E 02 15 1 .3 7 1 8 0 E 0?16 4 .^ 0 8 t o t
FRESH FEEDfll t t ■ n « 5 s 9 a n s i
10 2 .0 7 7 5 3 E 01 11 0 .0 12 6 .9 0 4 2 7 E 03 14 3 .4 4 2 9 7 E 02 15 1 .3 3 6 0 9 E «16 2 .5 6 8 8 2 E
RECYCLE f e e o01 17 1 .0 2 7 9 4 E 01
10 0 .0 11 0 .0 12 0 .0 14 0 .0 15 0 .016 0 .0
TO TAL NET FEED17 0 .0
10 2 .0 7 7 5 3 E 01 11 0 .0 12 6 .9 0 4 2 7 E 03 14 3 .4 4 2 9 7 E 02 15 1 .3 3 6 0>t15 2.S 6 8 8 2 E 01 T l 1 . 02794E 01
T C c o UnT IN G INFORMATION (FU SSF5 IM X61 FOLLOWS F O IT C Y tL E “ 2
01SCHARGE STREAM 1LOADING 10 9 .0 6 6 9 8 E 01 11 2 .6 1 3 6 4 E 00 12 3 .3 3 5 3 1 E 04 14 1 .5 3 8 1 8 E 03 15 5 .5 9 8 6 3 E 02
16 9 .& 6 7 2 3 E 01 17 4 .2 7 8 3 2 E 01 DISCHARGES 10 1 .7 9 2 0 4 E 01 11 •6.54577 E -0 1 12 6 .7 6 8 9 7 E 03 14 3 .7 7 5 4 4 E 02 15 1 .4 0 7 7 7 E 02
*6 2 .2 8 5 8 0 E 01 17 1 .0 7 4 9 2 E 01
rRfcSH ru c L HrfcD S IR t» H 1FRESH FEED 10 2 .0 7 3 9 5 E 01 11 0 .0 12 6 .8 9 2 4 1 E 03 14 0 .0 15 0 .0
16 0 .0 17 0 .0
J-RESH f-UEL FEED STREAM 2 FRESH FEED 10 0 .0 11 0 .0 12 0 .0 14 0 .0 15 0 .0
16 0 .0 1 r 0 .0 .............
FRESH FUEL FEED STREAM 3 FRESH FEEO 10 0 .0 11 0 .0 12 0 .0 14 0 .0 15 0 .0
1 6 975 17 JOT
FRESH FUEL FEEO STREAM 4FRESH FEEO________________ 10 0 .0 __________________11 0 .0 __________________12 0 .0 __________________14 0 .0 __________________15 0 .0
16 0 .0 17 0 .0
FRESH FUEL FEED STREAM 5 FRESH FEEO 10 0 .0 11 0 .0 12 0 .0 14 0 .0 *5 0 .0
16 0 .0 17 0 .0
MAKEUP STREAM RECYCLE FEEO
110 0 .0 11 0 .0 12 0 .0 14 1 .0 3 2 9 4 E 02 15 3 .9 1 6 S 4 E 01
16 6 .6 7 8 3 6 E TO TAL NET FEEP
00 17 3 .0 0 9 1 4 E 00 10 2 .5 6 3 4 2 E 00 11 0 .0 12 8 .5 1 8 9 5 E 02 14 1 .0 2 8 8 1 E 02 15 3 .9 0 1 17E Oj
16 6 .6 5 1 6 4 C 00 1 7 ' 2 .9 9 7 1 0 E 00
MAKEUP STREAM RECYCLE FEEO
210 0 .0 11 0 .0 12 0 .0 14 1 .1 8 1 2 8 E 02 15 4 .4 7 9 3 3 E 0]
16 7 .6 3 7 4 3 E TOTAL NET FEED
00 i t 3 .4 4 1 2 8 E 00 10 2 .6 8 0 1 8 E 00 11 0 .0 12 8 .9 0 7 2 9 E 02 14 1 .1 7 6 5 5 E 02 15 4 .4 6 1 42E 01
16 Y.6& 688E 60 1? 3 . ' 7 5 1 T O O
MAKEUP StREAM RLCYCLE FEEO
i10 0 .0 11 0 .0 12 0 .0 14 1 .3 8 5 3 7 E 02 15 5 .2 5 3 2 6 E 01
16 8.9& 700E TOTAL NET FEED
00 17 4 .0 3 5 8 5 E 00 10 2 .5 8 3 9 1 E 00 11 0 .0 12 8 .5 8 7 3 3 E 02 14 X .3 7 9 8 3 E 02 15 5 .2 3 2 2 4 E 01
16 8 .9 2 1 17E 00 17 4 . 01971E 06
MAKEUP STREAM RECYCLE FEEO
410 0 .0 11 0.0 12 0.0 14 0.0 15 0 .0
16 OiO TOTAL NET FEED
T T 1T.0 10 2 .6 0 6 8 5 E 00 11 0.0 12 8 .6 6 3 3 8 E 02 14 0.0 15 0.0
l 6 0 .0 17 0 .0
MAKEUP STREAM RECYCLE FEEO
S10 0 .0 11 0 .0 12 0.0 14 0.0 15 0 .0
16 0 .0 TOTAL NET FEED
17 0 .010 2 .7 6 2 6 1 E 00 11 0 .0 12 9 .1 8 1 2 S E 02 14 0.0 15 0 .0
0 .0 T 7 0 .0 ”
HKKEUP TIRE AW RECYCLE FEEO
610 0 .0 11 0 .0 12 0.0 14 0.0 15 0.0
.16 0 .0 TOTAL N ET FEEO
17 O .o 10 2 . 8Q400E 00 11 0.0 12 9 .3 1 8 6 5 E 02 14 0.0 15 0.0
16 0 .0 17 OrO
POKED? STREAM' RECYCLE FEED
110 0 .0 11 , 0 .0 12 0 .0 14 0.0 15 0.0
16 0 .0 TOTAL NET FEED
17 0.0 10 4 .7 0 7 0 7 E 00 11 0 .0 12 1 .5 6 4 2 9 E 03 14 0 .0 15 0 .0
— r& o.o----------------- r? o.o-------
**********TQ TALS SOHHEtTOVER "STOEIH S
Loaorae16 9 .2 6 7 2 3 E 01
10 9 .0 3 6 9 6 E 01.....17 4 .2 7 8 3 2 E 01
11 2.613*46 00_ - i r
3 .4 3 5 3 1 E 04 14 1 .5 3 8 1 8 E 03 15 5 .5 9 8 6 3 E 02
Oi&cHAkGE£16 2 .2 S »8 0 E 01
10 1 . V^Z04fc 01 17 1 .0 7 4 9 2 E 01
11 6.54577E-<11 6.76e4VE 03 14 3 .7 7 5 4 4 E 02 15 1 .4 0 7 7 7 E 02
Fr ESH FEEO 16 0 .0
10 2.0?395fe 01 17 0 .0
11 O.o 12 6 .8 9 2 4 1 E 03 14 0.0 15 0.0< e £ y c l£ FEEO
16 2 .3 2 7 2 8 E 0110 0 .0 "
17 1 .0 4 8 6 3 E 0111 O.o ~ n r 0.0 14 3 .5 9 9 5 8 E 02 15 1.3 6 4 9 4 E 02
r n T w n i E r 'F t e D16 2 .3 1 7 9 7 E 01
10 2.07O 8OE 01 17 1 .0 4 4 4 3 E 01
11 O.o 12 6 .8 8 1 4 6 E 03 14 3 .5 8 5 1 9 E 02 15 1 .3 5 9 4 8 E 02
ACCOUNTING INFORMATION (MASSES IN KC) FOLLOWS FOR CYCLE 3
P1SCHAR6E S TR E W 1_______________________________________________________________________________________________________________________ _________________LOADING 10 8 .7 C T3 1 E 01 T I 3 .2 9 2 6 9 E 00 12 3 .3 1 6 9 8 E 04 14 1 .5 6 4 3 4 E 03 15 5 .5 4 1 0 8 E 02
16 8 .6 1 6 6 3 E 01 1 7 4 .1 9 9 0 1 E 0 1 _______________________________________________________________________________________________DISCHARGES 10 1 .6 7 1 2 3 1 01 U 9 .1 7 9 5 6 E -0 1 12 6 .7 0 1 5 3 E 03 14 3 .9 2 2 2 9 E 02 15 1 .4 4 5 7 3 E 02
16 2 .1 9 3 0 4 E 01 17 1 .0 9 3 1 8 E 0 1 ________________ _______________________________________________________________________________________
END FUEL HANA6EHENT FOR CYCLE 3 _______________________________________________________________________________________
CYCLE 3 REQUIRED 1 .0 9 1 MINUTES CPU T IM E . AND 1 2 .7 8 2 M INUTES CLOCK TIM E ________________________________________________
END OF CASE - TOTAL CPU TIM E WAS 1 .8 0 .M INUTES TOTAL CLOCK T IM E MAS 2 2 .4 4 M INUTES____________________________________*** **44*# •**••••******••*•*•*•**********«***•*•* * * «********************«*******************«*9***************** ******* ****************** *********fr***************«************************************************************
♦♦♦♦♦♦♦♦♦THIS JOB WAS RUN ON 0 3 -1 0 -7 2 ON THE IBM 3 6 0 / 9 1 * ♦ * * »«»♦ »
W B'E N D E ITN O R N A LLY
297
REFERENCES
1. J. A. Davis and S. I. Kaplan, "Transport Synthesis," WARD-T-I8U9,USAEC Report, Bettis Atomic Power Laboratory (1965).
2. Argonne Code Center: Benchmark Problem Book, ANL-7^l6.
3. J. D. Jenkins, "Compilation of Standard Cores," Volume I, KAPL-M-JDJ-1, USAEC Report, Knolls Atomic Power Laboratory (1963).
B. J. Goulding, M. W. Croft et. al., "1000 Mw(e) LMFBR Follow-On Study," BAW-1328, USAEC Report, Babcock and Wilcox Company (1969)*
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