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C-1
Columns:
Are compression members which are subjected to concentric axial
compressive forces. These are to be found in trusses and as a lateral
bracing members in frame building. Short columns are sometimes
referred to as to as struts orstanchions.
Beam-Columns:Are members subjected to combined axial compressive
and bending stresses; These are found in single storey of
multi-storey framed structures. These are treated
independently in this course (chap. 12 in your text book).
Columns Theory:Stocky columns (short) fail by yielding of the material at
the cross section, but most columns fail by buckling at
loads for less then yielding forces.
P
P
P
P
(a) (b)
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C-2
For slender columns, Euler (1759) predicted the critical buckling load (Pcr)
also known as Euler Buckling Load as:
)1(2
2
CL
EIPcr
where: E = Young Modulus of Elasticity.
I = Minor moment of Inertia.
L = Unbraced length of column.
Derivation of Euler Buckling Load:
0"
2
2
yEI
Py
EI
M
dx
yd
cr
Solution of this differential equation:
y = A cos (cx) + B sin (cx)
where:
, A and B are constants.
EI
Pc
cr
x
L
y
x
y
Pcr Pcr
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C-3
From boundary conditions:
y = 0 @ x = 0, and
y = 0 @ x = L, we get (A = 0) and (B sin cL = 0)
if B 0, then cL = n where n = 0, 1, 2, 3
cL =
)(
/
2
2
2
2
22
2
2
C
rL
EA
L
ArE
L
EIP
LEI
P
cr
cr
2
2
g
cr
cr
rL
E
A
PF
---- Euler Buckling Critical Load
where: r = minor radius of gyration
The critical buckling load
is a function of the sectionproperties (A, L, r) and the
modulus of elasticity for
material, and is not a
function of the strength or
grade of the material.
Note:
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C-4
Example C-1
Find the critical buckling load for W 12 x 50, supported in a pinned-pinnedcondition, and has an over-all length of 20 feet?
Solut ion:
22
r
Lcr
EF
rmin = ry = 1.96 inch (properties of section).
ksiFcr 19
290002
96.11220
2
Note:
The steel grade is not a factor affecting buckling.
Pcr= FcrA = 19.1 x 14.7 = 280.8 kips
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For short (stocky) columns; Equation (C-2) gives high values for
(Fcr), sometimes greater then proportional limit, Engessor (1889)proposed to use (Et) instead of (E) in Euler formula:
)3(2
2
CL
IEP tcr
where:
Et = Tangent Modulus of Elasticity
Et < E
When (Fcr) exceeds (FPR), this is called
Inelastic Buckling, constantly variable
(Et) need to be used to predict (Fcr)
in the inelastic zone.
Shanley (1947), resolved this inconsistency.
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C-6
Depending on (L/r) value the column buckling
strength was presented as shown by Shanley.
Residual Stresses:-
Due to uneven cooling of hot-rolled sections,
residual stresses develop as seen here.
The presence of residual stresses in almost all
hot-rolled sections further complicates the issue
of elastic buckling and leads towards inelastic
buckling.
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C-7
The Previous conditions are very
difficult to achieve in a realistic building
condition, especially the free rotation of pinnedends. Thus an effective slenderness factor is
introduced to account for various end
conditions:
Thus:
4
2
2
CE
F
rKL
cr 2
rK l
t
2
cr
EFor,
where:
K = Effective length factor.(Kl) = Effective length.
(Kl/r) = Effective slenderness ratio.
see commentary
(C C2.2) (page 16.1-240)
The Euler buckling formula (C-1) is based on:
1 Perfectly straight column. (no crookedness).
2 Load is concentric (no eccentricity).
3 Column is pinned on both ends.
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C-7
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C-7
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C-7
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C-8
AISC (Chapter E) of LRFD code stipulates:
Pu (factored load) c Pn
where:
Pu = Sum of factored loads on column.
c = Resistance factor for compression = 0.90
Pn = Nominal compressive strength = FcrAg
Fcr= Critical buckling Stress. (E3 of LFRD)
a) for
3.4-E
EF
3.3-E0.877FF
0.44FFor4.71
r
Kl
3.2-EF0.658F
0.44FFor4.71r
Kl
2
rK L
2
e
ecr
yeF
E
ycr
yeF
E
y
eF
yF
y
b) for
where:
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C-9
The above two equations of the LRFD code can be
illustrated as below:
where:
E
F
r
Kl
y
c
* The code further stipulates that an upper value for
for column should not exceed (200).
* For higher slenderness ratio,
Equation (E-3.3) controls and
(Fy) has no effect on (Fcr).
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C-10
Determine the design compressive strength (cPn) of W 14x74 with an
untraced length of (20 ft), both ends are pinned, (A-36) steel is used?
Example C-2
Solution:
ksi30.56(96.77)
x2900
r
Kl
EFe
(0k)20096.772.48
240
r
Kl
2
2
2
2
max.
ksi21.99360.611
36x(0.658)F0.658F 1.178yF
F
cre
y
Kl =1 x 20 x 12 = 240 in
Rmin = ry = 2.48
0.44 Fy = 0.44 x 36 =15.84 ksi
Fe 0.44 Fy Equ. E-3.2
(controls)
c Pn = 0.9 x Fcrx Ag = 0.9 x (21.99) x 21.8
= 433.44 kips (Answer)
Also from (table 4-22) LFRD Page 4-320
c Fcr= 19.75 ksi (by interpolation)
c Pn = c FcrAg = 430.55 kips
(much faster)
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C-11
For must profiles used as column, the buckling of thin elements in the section may
proceed the ever-all bucking of the member as a whole, this is called local bucking.To prevent local bucking from accruing prior to total buckling. AISC provides upper
limits on width to thickness ratios (known as b/t ratio) as shown here.
See AISC (B4)
(Page 16.1-14)
See also:Part 1 on properties
of various sections.
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C-12
Depending on their ( b/t ) ratios (referred to as ) ,
sections are classified as:a) Compact sections are those with flanges fully welded
(connected) to their web and their:
p (AISC B4)
b) Non compact Sections:pr (B4)
c) Slender Section:
> r (B4)
Certain strength reduction factors (Q) are introduced for slender
members. (AISC E7). This part is not required as most section
selected are compact.
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C-13
Example C-3
Determine the design
compressive strength
(c Pn) for W 12 x 65
column shown below,
(Fy = 50 ksi)?
From properties:
Ag =19.1 in2rx = 5.28 in
ry = 3.02 inksi40.22550x0.8045
F0.658F
3.2)(EEqu.ksi)22(F0.44F
ksi96.2(54.55)
x29000
r
KlEF
31.795.28
12x8x1
r
LK
54.555.28
12x24x1
r
LK
y
96.2
50
cr
ye
2
2
2
2
e
y
yy
x
xx
Solut ion:
c Pn = 0.9 x FcrAg = 0.9 x 40.225 x 19.1 = 691.5 kips
A) By direct LRFD
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C-14
B) From Table (4.22) LRFD
Evaluate = = 54.55
Enter table 4.22 (page 4 318 LRFD)
cFc = 36.235 ksi (by interpolation)
Pn = Fc x Ag = 692.0 kips
C) From (Table 4.1 LRFD)
maxrKl
ft13.7
1.75
1x24
r
r
LK(KL)
y
x
xxy
Enter table (4.1 ) page 4.17 LFRD with (KL)y = 13.7
Pn = 691.3 kips (by interpolation).
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C-15
Design with Columns Load Table (4) LFRD:-
A) Design with Column Load Table (4) LFRD:The selection of an economical rolled shape to resist a given
compressive load is simple with the aid of the column load tables.
Enter the table with the effective length and move horizontally until
you find the desired design strength (or something slightly larger). In
some cases, Usually the category of shape (W, WT, etc.) will have
been decided upon in advance. Often the overall nominal
dimensions will also be known because of architectural or other
requirements. As pointed out earlier, all tabulated values correspond
to a slenderness ratio of 200 or less. The tabulated unsymmetricalshapes the structural tees and the single and double-angles
require special consideration and are covered later.
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C-16
EXAMPLE C - 4
A compression member is subjected to service loads of 165 kips dead loadand 535 kips live load. The member is 26 feet long and pinned in each end.
Use (A572 Gr 50) steel and select a W14 shape.
SOLUTION Calculate the factored load:
Pu = 1.2D + 1.6L = 1.2(165) + 1.6(535) = 1054 kips
Required design strength cPn = 1054 kips
From the column load table for KL = 26 ft, a W14 176
has design strength of 1150 kips.
ANSWER
Use a W14 145, But practically W14 132 is OK.
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C-17
EXAMPLE C - 5Select the lightest W-shape that can resists a factored compressive load Pu of
190 kips. The effective length is 24 feet. Use ASTM A572 Grade 50 steel.
SOLUTION
The appropriate strategy here is to fined the lightest shape for each nominal
size and then choose the lightest overall. The choices are as follows.
W4, W5 and W6: None of the tabulated shape will work.W8: W8 58, cPn = 194 kips
W10: W10 49, cPn = 239 kips
W12: W12 53, cPn = 247 kips
W14: W14 61, cPn = 276 kips
Note that the load capacity is not proportional to the weight (or cross-sectional area). Although the W8 58 has the smallest design strength of
the four choices, it is the second heaviest.
ANSWER Use a W10 49.
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C-18
B) Design for sections not from Column Load Tables:
For shapes not in the column load tables, a trial-and-error approach must be used.The general procedure is to assume a shape and then compute its design strength. Ifthe strength is too small (unsafe) or too large (uneconomical), another trial must bemade. A systematic approach to making the trial selection is as follows.
1) Assume a value for the critical buckling stress Fcr. Examination of AISC Equations
E3-2 and E3-3 shows that the theoretically maximum value of Fcr is the yield stress Fy.
2) From the requirement that cPn Pu, let
cAgFcr Pu and
3) Select a shape that satisfies this area requirement.
4) Compute Fcrand cPn for the trial shape.
5) Revise if necessary. If the design strength is very close to the required value,the next tabulated size can be tried. Otherwise, repeat the entire procedure,
using the value of Fcrfound for the current trial shape as a value for Step 1
6) Check local stability (check width-thickness ratios). Revise if necessary.
crc
u
F
P
gA
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C-19
3.2.EEqu.LRFD(15.84)F0.44F
ksi22.9111.8
x29000
r
Kl
EF
ye
2
2
2
2
e
Example C-6
Select a W18 shape of A36 steel that can resist a factored load of 1054 kips.
The effective length KL is 26 feet.
Solut ion:Try Fcr= 24 ksi (two-thirds of Fy):
Required2848
2490
1054in
F
PA
crc
ug .
)(.
Try W18 x 192:Ag = 56.4 in
2 > 48.8in2
(OK)200111.82.79
26(12)
r
KL
min
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C-20
(OK)..
)(
r
KL
in62.83.in.A
:234xTry W18
in.).(.
ARequired
:192)xW18theforcomputedjustvalue(theksi.FTry
(N.G.)
105494318.64x56.4x0.9FA0.9P
ksi18.64
36x0.532x360.658F0.658F
min
2g
2g
cr
kkipscrgnc
yF
F
cr
22.9
36
e
y
2005109852
1226
868
8362641890
1054
6418
2
crc
u
F
P
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C-21
234xW18aUseAnswer
(OK)42.236
25313.8t
h
(OK)15.836
952.8
2t
b
:cheackedbemustratios
thicknes-widththesotables,loadcolumntheinnotisshapeThis
(OK)1054118519.15x68.8x0.9FA0.9P
ksi19.1536x0.53236x0.658F0.658F
3.2)-(Equ.ELFRDUse0.44FF
23.87ksi
109.5
29000EF
w
f
f
kkips
crgnc
y
F
F
cr
ye
2
2
2
r
Kl
2
e
23.87
36
e
y
COMPRESSIVE STRENGTH FOR TORSIONAL AND
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C-21
COMPRESSIVE STRENGTH FOR TORSIONAL AND
FLEXURAL-TORSIONAL BUCKLING OF MEMBERS
WITHOUT SLENDER ELEMENTS
This section applies to singly symmetric and unsymmetric members, and certaindoubly symmetric members, such as cruciform or built-up columns with compact
and noncompact sections
For double-angle and tee-shaped compression members:
where Fcry is taken as Fcr from Equation E3-2 or E3-3, for flexural buckling
about the y-axis of symmetry and KL/r= KL/ry, and
COMPRESSIVE STRENGTH FOR TORSIONAL AND FLEXURAL
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C-21
COMPRESSIVE STRENGTH FOR TORSIONAL AND FLEXURAL-
TORSIONAL BUCKLING OF MEMBERS WITHOUT SLENDER ELEMENTS
COMPRESSIVE STRENGTH FOR TORSIONAL AND FLEXURAL
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C-21
COMPRESSIVE STRENGTH FOR TORSIONAL AND FLEXURAL-
TORSIONAL BUCKLING OF MEMBERS WITHOUT SLENDER ELEMENTS
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C-21
Single angle compression membera) For equal-leg angles or unequal-leg angles connected through the longer leg that
are individual members or are web members of planar trusses with adjacent web
members attached to the same side of the gusset plate or chord:
For unequal-leg angles with leg
length ratios less than 1.7 and
connected through the shorter leg,
KL/r from Equations E5-1 and E5-
2 shall be increased by adding
4[(bl /bs )2
1], but KL/r of themembers shall not be less than
0.95L/rz .
where
L = length of member between work points at truss chord centerlines,
in. (mm)
bl = longer leg of angle, in. (mm)bs = shorter leg of angle, in. (mm)
rx = radius of gyration about geometric axis parallel to connected leg,
in. (mm)
rz = radius of gyration for the minor principal axis, in. (mm)
Si l l i b
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C-21
Single angle compression member
(b) For equal-leg angles or unequal-leg angles connected through the longer leg that
are web members of box or space trusses with adjacent web membersattached to the same side of the gusset plate or chord:
For unequal-leg angles with leg
length ratios less than 1.7 and
connected through the shorter
leg, KL/r from Equations E5-3
and E5-4 shall be increased by
adding 6[(bl /bs )2 1], but KL/r
of the member shall not be less
than 0.82L/rz ,
where
L = length of member between work points at truss chord centerlines,
in. (mm)
bl = longer leg of angle, in. (mm)bs = shorter leg of angle, in. (mm)
rx = radius of gyration about geometric axis parallel to connected leg,
in. (mm)
rz = radius of gyration for the minor principal axis, in. (mm)
Si l l i b
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C-21
Single angle compression member
(b) For equal-leg angles or unequal-leg angles connected through the longer leg that
are web members of box or space trusses with adjacent web membersattached to the same side of the gusset plate or chord:
For unequal-leg angles with leg
length ratios less than 1.7 and
connected through the shorter
leg, KL/r from Equations E5-3
and E5-4 shall be increased by
adding 6[(bl /bs )2 1], but KL/r
of the member shall not be less
than 0.82L/rz ,
where
L = length of member between work points at truss chord centerlines,
in. (mm)
bl = longer leg of angle, in. (mm)bs = shorter leg of angle, in. (mm)
rx = radius of gyration about geometric axis parallel to connected leg,
in. (mm)
rz = radius of gyration for the minor principal axis, in. (mm)