NODAL AND LOOP ANALYSIS TECHNIQUES LEARNING GOALS CIRCUITS WITH OPERATIONAL AMPLIFIERS Develop systematic techniques to determine all the voltages and currents in a circuit NODAL ANALYSIS LOOP ANALYSIS Op-amps are very important devices, widely available, that permit the design of very useful circuit… and they can be modeled by circuits with dependent sources
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NODAL AND LOOP ANALYSIS TECHNIQUES
LEARNING GOALS
CIRCUITS WITH OPERATIONAL AMPLIFIERS
Develop systematic techniques to determine all the voltagesand currents in a circuit
NODAL ANALYSISLOOP ANALYSIS
Op-amps are very important devices, widely available,that permit the design of very useful circuit…
and they can be modeled by circuits with dependent sources
NODE ANALYSIS
• One of the systematic ways to determine every voltage and current in a circuit
The variables used to describe the circuit will be “Node Voltages” -- The voltages of each node with respect to a pre-selected reference node
IT IS INSTRUCTIVE TO START THE PRESENTATION WITHA RECAP OF A PROBLEM SOLVED BEFORE USING SERIES/PARALLEL RESISTOR COMBINATIONS
COMPUTE ALL THE VOLTAGES AND CURRENTS IN THIS CIRCUIT
SECOND: “BACKTRACK” USING KVL, KCL OHM’S
k
VI a
62 :SOHM' 13 2KCL: I I I
4
34
*4124
12
IkV
II
b
5
345
*3
0
IkV
III
C
:SOHM'
:KCL
k12kk 12||4
k6
kk 6||6
k
VI
12
121
)12(93
3
aV
3I
FIRST REDUCE TO A SINGLE LOOP CIRCUIT
THE NODE ANALYSIS PERSPECTIVETHERE ARE FIVE NODES. IF ONE NODE IS SELECTED AS REFERENCE THEN THERE AREFOUR VOLTAGES WITH RESPECTTO THE REFERENCE NODE
THEOREM: IF ALL NODE VOLTAGES WITHRESPECT TO A COMMON REFERENCE NODEARE KNOWN THEN ONE CAN DETERMINE ANY OTHER ELECTRICAL VARIABLE FORTHE CIRCUIT
aS
aS
VVV
VVV
1
10
ba
ba
VVV
VVV
3
3 0
______caV
QUESTIONDRILL
REFERENCE
aV
bV
cV
KVL KVL
WHAT IS THE PATTERN???
KVL
05 bc VVV
ONCE THE VOLTAGES ARE KNOWN THE CURRENTS CANBE COMPUTED USING OHM’SLAW
A GENERAL VIEW
Rv
NmR vvv
5 cbV V V
THE REFERENCE DIRECTION FOR CURRENTS IS IRRELEVANT
'i
Rv
USING THE LEFT-RIGHT REFERENCE DIRECTIONTHE VOLTAGE DROP ACROSS THE RESISTOR MUSTHAVE THE POLARITY SHOWN
R
vvi Nm LAW SOHM'
IF THE CURRENT REFERENCE DIRECTION IS REVERSED ...
'Rv
THE PASSIVE SIGN CONVENTION WILL ASSIGNTHE REVERSE REFERENCE POLARITY TO THE VOLTAGE ACROSS THE RESISTOR
R
vvi mN 'LAW SOHM'
'ii PASSIVE SIGN CONVENTION RULES!
DEFINING THE REFERENCE NODE IS VITAL
SMEANINGLES IS4V VSTATEMENT THE 1 UNTIL THE REFERENCE POINT IS DEFINED
BY CONVENTION THE GROUND SYMBOLSPECIFIES THE REFERENCE POINT.
V4
ALL NODE VOLTAGES ARE MEASURED WITHRESPECT TO THAT REFERENCE POINT
V2
_____?12 V
12V
THE STRATEGY FOR NODE ANALYSIS 1. IDENTIFY ALL NODES AND SELECT A REFERENCE NODE
2. IDENTIFY KNOWN NODE VOLTAGES
3. AT EACH NODE WITH UNKNOWN VOLTAGE WRITE A KCL EQUATION(e.g.,SUM OF CURRENT LEAVING =0)
0:@321 IIIV
a
4. REPLACE CURRENTS IN TERMS OF NODE VOLTAGES
0369
k
VV
k
V
k
VV baasa AND GET ALGEBRAIC EQUATIONS IN THE NODE VOLTAGES ...
REFERENCE
SV
aV
bV
cV
0:@543 IIIV
b
0:@65 IIV
c
0943
k
VV
k
V
k
VVcbbab
039
k
V
k
VVcbc
SHORTCUT:SHORTCUT: SKIP WRITING THESE EQUATIONS...
AND PRACTICE WRITING
THESE DIRECTLY
a b c
d
aV
bV
cV
dV
1R 3R
2R
WHEN WRITING A NODE EQUATION...AT EACH NODE ONE CAN CHOSE ARBITRARYDIRECTIONS FOR THE CURRENTS
AND SELECT ANY FORM OF KCL.WHEN THE CURRENTS ARE REPLACED IN TERMSOF THE NODE VOLTAGES THE NODE EQUATIONSTHAT RESULT ARE THE SAME OR EQUIVALENT
00321
321
R
VV
R
VV
R
VVIII cbdbba
0LEAVING CURRENTS
00321
321
R
VV
R
VV
R
VVIII cbdbba
0 NODE INTO CURRENTS
2I3I1I
a b c
d
aV
bV
cV
dV
1R 3R
2R '2I
'3I'
1I
00321
'3
'2
'1
R
VV
R
VV
R
VVIII bcdbab
0LEAVING CURRENTS
00321
'3
'2
'1
R
VV
R
VV
R
VVIII bcdbab
0 NODE INTO CURRENTS
WHEN WRITING THE NODE EQUATIONSWRITE THE EQUATION DIRECTLY IN TERMSOF THE NODE VOLTAGES.BY DEFAULT USE KCL IN THE FORMSUM-OF-CURRENTS-LEAVING = 0
THE REFERENCE DIRECTION FOR THECURRENTS DOES NOT AFFECT THE NODEEQUATION
CIRCUITS WITH ONLY INDEPENDENT SOURCES
HINT:HINT: THE FORMAL MANIPULATION OF EQUATIONS MAY BE SIMPLER IF ONE USES CONDUCTANCES INSTEAD OF RESISTANCES.
@ NODE 1
02
21
1
1
R
vv
R
viA SRESISTANCE USING
0)( 21211 vvGvGiA ESCONDUCTANC WITH
REORDERING TERMS
@ NODE 2
REORDERING TERMS
THE MODEL FOR THE CIRCUIT IS A SYSTEMOF ALGEBRAIC EQUATIONS
THE MANIPULATION OF SYSTEMS OF ALGEBRAICEQUATIONS CAN BE EFFICIENTLY DONEUSING MATRIX ANALYSIS
LEARNING BY DOING
@ NODE 1 WE VISUALIZE THE CURRENTSLEAVING AND WRITE THE KCL EQUATION
REPEAT THE PROCESS AT NODE 2
03
12
4
122
R
vv
R
vvi
OR VISUALIZE CURRENTS GOING INTO NODE
WRITE THE KCL EQUATIONS
mA15
A
B
C
k8 k8k2 k2
SELECT ASREFERENCE
AV
BV
MARK THE NODES (TO INSURE THAT NONE IS MISSING)
ANOTHER EXAMPLE OF WRITING KCL
WRITE KCL AT EACH NODE IN TERMS OFNODE VOLTAGES 015
82@ mA
k
V
k
VA AA
01528
@ mAk
V
k
VB BB
A MODEL IS SOLVED BY MANIPULATION OFEQUATIONS AND USING MATRIX ANALYSIS
THE NODE EQUATIONS
kRRkR
mAimAi BA
6,12
4,12
321
THE MODEL
REPLACE VALUES AND SWITCH NOTATIONTO UPPER CASE
NUMERICAL MODEL
USE GAUSSIAN ELIMINATION
ALTERNATIVE MANIPULATION
k12/*
k6/*
242
1223
21
21
VV
VV
RIGHT HANDSIDE IS VOLTS.COEFFS ARENUMBERS
][122 1 VV ADD EQS
equations) add (and3/*][604 2 VV
LEARNING EXAMPLE
SOLUTION USING MATRIX ALGEBRA
PLACE IN MATRIX FORM
USE MATRIX ANALYSIS TO SHOW SOLUTION
PERFORM THE MATRIX MANIPULATIONS
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A
AAdjA
FOR THE ADJOINT REPLACEEACH ELEMENT BY ITSCOFACTOR
AND DO THE MATRIX ALGEBRA ...
kkkV
6
104
3
10118
332
1
SAMPLE
AN EXAMPLE OF NODE ANALYSIS
1@v
2@ v
3@ v
Rearranging terms ...
2&1 BETWEEN ESCONDUCTANC
3&1 BETWEEN ESCONDUCTANC
3&2 BETWEEN ESCONDUCTANC
NODE TO CONNECTED ESCONDUCTANC
COULD WRITE EQUATIONS BY INSPECTION
WRITING EQUATIONS “BY INSPECTION”
FOR CIRCUITS WITH ONLY INDEPENDENTSOURCES THE MATRIX IS ALWAYS SYMMETRIC
THE DIAGONAL ELEMENTS ARE POSITIVE
THE OFF-DIAGONAL ELEMENTS ARE NEGATIVE
Conductances connected to node 1
Conductances between 1 and 2
Conductances between 1 and 3
Conductances between 2 and 3
VALID ONLY FOR CIRCUITSWITHOUT DEPENDENTSOURCES
k
VV
k
VmAV
1264:@ 211
1
USING KCL
0126
2:@ 1222
k
VV
k
VmAV
BY “INSPECTION”
mAVk
Vkk
412
1
12
1
6
121
mAVkkk
212
1
6
1
12
12
LEARNING EXTENSION
mA6
1I
062:@ 11 mAmAIVKCL
2I
3I
036
6:@ 222 k
V
k
VmAV
mAI
mAI
VV
4
2
12
3
2
2
CURRENTS COULD BE COMPUTED DIRECTLYUSING CURRENT DIVIDER!!
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kI
mAmAkk
kI
4)6(63
6
2)6(63
3
3
2
LEARNING EXTENSION
IN MOST CASES THEREARE SEVERAL DIFFERENTWAYS OF SOLVING APROBLEM
NODE EQS. BY INSPECTION
mAVVk
6202
121
mAVkk
V 63
1
6
10 21
k
VI
k
VI
k
VI
3622
32
21
1
CIRCUITS WITH DEPENDENT SOURCES CANNOTBE MODELED BY INSPECTION. THE SYMMETRYIS LOST.
A PROCEDURE FOR MODELINGA PROCEDURE FOR MODELING•WRITE THE NODE EQUATIONS USING DEPENDENT SOURCES AS REGULAR SOURCES.•FOR EACH DEPENDENT SOURCE WE ADD ONE EQUATION EXPRESSING THE CONTROLLING VARIABLE IN TERMS OF THE NODE VOLTAGES
02
21
1
1
R
vv
R
vio
02
12
3
2
R
vv
R
viA
MODEL FOR CONTROLLING VARIABLE
3
2
R
vio
NUMERICAL EXAMPLE
mAvkk
vk
vkk
vkk
23
1
12
1
6
1
06
1
3
2
6
1
12
1
21
21
0111
223
121
v
RRv
RR
REPLACE AND REARRANGE
AivRR
vR
2
321
2
111
k4/*
k6/*
][123
02
21
21
VVV
VV
ADDING THE EQUATIONS ][125 2 VV
VV5
241
CIRCUITS WITH DEPENDENT SOURCES LEARNING EXAMPLE
LEARNING EXAMPLE: CIRCUIT WITH VOLTAGE-CONTROLLED CURRENT
WRITE NODE EQUATIONS. TREAT DEPENDENTSOURCE AS REGULAR SOURCE
EXPRESS CONTROLLING VARIABLE IN TERMS OFNODE VOLTAGES
FOUR EQUATIONS IN OUR UNKNOWNS. SOLVEUSING FAVORITE TECHNIQUE
OR USE MATRIX ALGEBRA
REPLACE AND REARRANGE
CONTINUE WITH GAUSSIAN ELIMINATION...
USING MATLAB TO SOLVE THE NODE EQUATIONS
]/[2
,4,2,4
,2,1
4
321
VA
mAimAikR
kRRkR
BA
» R1=1000;R2=2000;R3=2000;R4=4000; %resistances in Ohm» iA=0.002;iB=0.004; %sources in Amps» alpha=2; %gain of dependent source
DEFINE THE COMPONENTS OF THE CIRCUIT
DEFINE THE MATRIX G » G=[(1/R1+1/R2), -1/R1, 0; %first row of the matrix-1/R1, (1/R1+alpha+1/R2), -(alpha+1/R2); %second row0, -1/R2, (1/R2+1/R4)], %third row. End in comma to have the echo