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8/13/2019 Eq Ckts Voltage Division Current Division
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1
Equivalent Circuits
Originalcircuit
I
V+
-
1
2
The Current Voltage (I-V) Relationshipdefines any element. It can also be used todefine any circuit in the box. We assumethe original circuit is complicated.
Equivalentcircuit
I
V
+
-
1
2
Replace original circuit with simplerequivalent circuit that exhibits the same I-Vrelationship (at nodes 1 & 2) !
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Circuit Simplification for Parallel Current Sources & ResistancesIS
VS R 1 R 2 R 3
IS1 IS2 IS3
IR1 IR2 IR3
IS
VS R 1
R 2 R 3IS1 IS2 IS3
IR1 IR2 IR3
Apply arbitrary voltage source Vs
Since all elements are in parallel, they alsohave Vs across them.We assign currents in red
KCL at top node I in = I out
IS + I S2 = I S1 + I R1 +I R2 +I R3 +I S3
Is = (I S1 -I S2+ I S3 )+I R1 +I R2 +I R3
IS= I STOT +I R1 + I R2 + I R3
ISTOT -
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Continued..
IS
VS R 1 R 2 R 3
ISTOT
IR1 IR2 IR3
Therefore, the ckt can be redrawn asshow on the left where:
IS= I STOT +V S(1/R 1 + 1/R 2 + 1/R 3)
IS= I STOT +V S(1/R TOTAL )
321 /1/1/11
R R R R TOTAL
N
i i
TOTAL
R
R
1
11
IS
VSRTOTALISTOT
+
-
VS
Resistors in parallel
1. So we can simply add curr ent sources in paral lel bu t consideri ng theirorientation* For th is problem, Curr ent sour ces point in g down are posit ive (I s1 and I s3) thosepoint in g up are negative (Is2)2. And we can combine paral lel r esistors
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Numeric ExampleIS
VS 6K 3K1A 3A 10A
2K
IS
VS RTOTALISTOT
+
-
VS
Find Circuit 2 that is equivalent toCircuit 1
ISTOT = 1 + 10 3 = 8 A K
K K K R TOTAL 1
)3/1()2/1()6/1(1
IS = 8A +V S/1K=IS = (1/1K)V S + 8A
I S
V S
1/1K=slopey = mx + b
8 A
- 8000 V
Circuit 1
Circuit 2
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Similar Numeric ExampleIS
VS 6K 3K1A 3A 10A
2K
IS
VS RTOTISTOT
+
-
VS
Find Circuit 2 that is equivalent toCircuit 1 ( changing the orientation ofIsTOT ):ISTOT = -1 - 10 + 3 = -8 A
K K K K RTOTAL 1)3/1()2/1()6/1(
1
Circuit 1
Circuit 2
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Last Numeric ExampleIS
VS 12K 6K
-3A 4A -5A12K
IS
VS RTOTISTOT
+
-
VS
Find Circuit 2 that is equivalent to Circuit 1:ISTOT = -(-3A) (4A) + (-5A)= -6A
K K K K RTOTAL 3)6/1()12/1()12/1(
1
Circuit 1
Circuit 2
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Circuit Simplification for Series Voltage Sources & Resistances
IS R 1VS1
+
-
VS
R 2
R 3
VS2
VS3IS
Is there a way to combine series resistances and voltage sources in the gray box (circuit on the
left)? The resulting simplified circuit will be in the form of the circuit on the right.
Apply arbitrary current source I S. I S is the only current in the circuit; it enters and leaves allof these elements in series.
KVL gives us:-V S + V S1 + R 1IS VS2 + R 2I S +V S3 + R 3I S = 0
-V S + (V S1 VS2 +V S3) + R 1I S + R 2IS + R 3I S = 0
Algebraic properties allows us to change the order of the items in the circuit and in theequation, so we can rewrite it as
-V S + V STOTAL + I S(R 1+R 2+R 3) =0
VSTOTAL
IS
RTOTAL
VSTOTAL
+
-
VS
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Continued..-V S + V STOTAL + I S(R 1+R 2+R 3) =0
Now solving the previous equation for I S:
321 R R R R TOTAL
N
i
iTOTAL R R1
IS
RTOTALV
TOTAL
+
-
VS Resistors in series
* * * 1. So we can simply add voltage sources in series but consider in g their ori entation* * * 2. Simply add series resistors together
TOTAL
STOTALS
TOTAL
STOTALS S R
V V
R R R RV
V R R R
I
1)(
1
321321
This gives us Linear relationship such asy = mx + b
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Numeric Example
Find V TOTAL and R TOTAL so that the circuit on the right has the same I-V
characteristic as the circuit on the left??
We add R TOTAL = 2K + 5K + 7K = 14KVSTOTAL = -6V -3V + 15V = 6V
IS 2K6V
+
-
VS
5K
7K
3V
15V
IS
RTOTAL
VSTOTAL
+
-
VS
IS
14K
6V
+
-
VS
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Numeric Example
How to Find Vs and Rs so that the circuit on the right has the same I-V
characteristic as the circuit on the left??
VS2
VS1R 1
VS3R 2
VSTOTAL
R TOTAL
A
B
A
B
For V S1 = 3V, R 1 = 5K, V S2 = 7V, R 2 = 2K and V S3 = 11VWe add R TOT = 5K + 2K =7KVTOT = 3V -7V -11V = -15V
Pay attention to the sign of the final voltage source in the final circuit!
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Series/Parallel Reduction of Resistance
R 1
R 2
R 3
R 4
A
B
I3
I3
R 1
R 2
R 3
R 4
A
B
R TOTAL
A
B
R 1
R 2 R 34
Find R TOTAL
Step 1: Working with only 2 resistors at a time, start
opposite ports A and B R 3 and R 4 are in series R 34 = R 3 + R 4
Step 2: Next we see that R 2 and R 34 have the sameendpoints (ie share the same voltage)
R 34 // R 2 = R 234
Step 3: R 1 is in series with R 234 .Therefore R TOT = R 1 + R 234 .
R TOTAL = R 1 + (R 2//(R 3+R 4))
R1
R234
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Example Series/Parallel Reduction of Resistance
R 3=1
A
B
R TOTAL
A
B
R 4=5R 2=3
R 1=8
R 34 =6
R 1=8
R 2=3
Find R TOTAL
Step 1:R 3 and R 4 are in series R 34 = 1 + 5 =6New equivalent resistance gets connected across same 2 nodes
Step 2: R 2 and R 34 have the same endpoints (ie share the samevoltage)
R 34 // R 2 = R 234R 234 =6//3= 1/{(1/6)+(1/3)}=2
New equivalent resistance gets connected across same 2 nodes
Step 3: R 1 is in series with R 234 . Therefore, R TOT = R 1 + R 234 .R TOTAL = R 1 + (R 2//(R 3+R 4))= 8+2 = 10 ohms
R1=8
R234 =2
Step 1:
Step 2:
Step 3:
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14
Voltage Division
Consider two resistors in series with a voltageacross them:
R 1
R 2
v 1
+
+
v 2
v s 21
11 R R
Rvv s
21
22 R R
Rvv s
+
KVL: - Vs + V1 +V
2 = 0
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Voltage DivisionChanging the orientation of the element voltages:
R1
R 2
v1
+
+
v 2
v s
21
11 R R
Rvv s
21
22 R R R
vv s+
+
_
+
vX
v Y
21
1
R R
Rvv s X
21
2
R R R
vv sY If we instead use v X, we make a sign change,since KVL still applies
KVL: - Vs + V 1 +V 2 = 0KVL: - Vs - V X -V Y = 0
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In General: Voltage Division
Consider N resistors in series :
Source voltage(s) are divided between the resistors in direct proportion to their resistances
N
j j
iS
i R
R
RV V
1
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Voltage Division- example 1
5
10
v 1
+
+
v 2
Vs=9V V V V
R R R
vv s 331
9105
5)9(
21
11
+
+
_
+
v X
v Y
V V V R R
Rvv s 6
32
9105
10)9(
21
22
V V R R
Rvv s X 3105
5)9(
21
1
V V R R
Rvv sY 6105
10)9(
21
2
KVL: -Vs + V 1 +V 2 = 0.KVL: -Vs - V X -V Y = 0. For the total voltages around the loop to equal zero, V X and V Y must be negative for this circuit! So apply negative sign in voltage dividers for V X and V Y .
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Voltage Division- example 2
10
30
v 1
+
+
v 2
Vs=12V V V V
R R R
vv s 341
123010
10)12(
21
11
+ +
_
+
v X
v Y
V V V R R
Rvv s 9
43
123010
30)12(
21
22
V V R R
Rvv s X 33010
10)12(
21
1
V V R R
Rvv sY 93010
30)12(
21
2
Note: The orientation of the source voltage has been flipped from previous example!
KVL: Vs + V 1 +V 2 = 0. For the total voltages around the loop to equal zero, V 1 and V 2 mustbe negative for this circuit! So apply negative sign in voltage dividers for V 1 and V 2 .KVL: Vs - V X -V Y = 0
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19
10
V s
5
+- Find I x , V S
I X
+ -10 V
20 30
Where to start?1) Try Ohms Law 2) Use the values found to write KVL or KCL3) Alternative: use voltage division
Example 1 similar to HW
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20
10
V s
5
+- Find I x , V S
I X +
++
+
--
-
-10 V
20 30
V 20
V 10
V 30
I 5 I 30
I 10
I S
Making assignments shown in blue
1) Ohms Lawassign I 5 so I 5 = - (10V/5 ) = - 2A (note not PSC)2)KCL at B : 0=I 5 + I 10 therefore I 10 = -(-2A) = 2A3) V 10 = I 10(10 ) = (2A)(10 )=20 V4) Cannot apply KCL yet to get other unknown currents
Example 1B
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21
10
V s
5
+- Find I x , V S
I X +
++
+
--
-
-10 V
20 30
V 20
V 10
V 30
I 5 I 30
I 10
I S
5) Instead apply KVL
+10+V 10-V 20=0 +10+20-V 20=0 V 20 = 30V6) I x=V 20 /20 = 30/20 = 1.5 A note: follows PSC7) KCL at A: I 5 = I S +I X IS=I 5 I X = (-2A)-1.5A = - 3.5A =I 30 8) V 30=I 30(30 ) = (-3.5A)(30 ) = -105 V9) KVL: +V S +V 30-V 20 =0 V S= V 20-V 30 =30-(-105) = 135 V
AExample 1
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22
10
V s
5
+- Find I x , V S
I X +
++
+
--
-
-10 V
20 30
V 20
V 10
V 30
I 5 I 30
I 10
I S
Alternative: Applying Voltage Division would have saved us steps
205105
5 V V V V V 30)5105(1020
Example 1
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Review: Voltage DivisionConsider two resistors in series with a voltage v
across them:
R1
R 2
v1
+
+
v 2
v s
21
11 R R
Rvv s
21
22 R R R
vv s+
+
_
+
vX
v Y
21
1
R R
Rvv s X
21
2
R R R
vv sY
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How do I know if I need to apply a negative signwhen using voltage division?
Answer: Pay attention to the orientation of the element voltages withrespect to the source voltages, knowing that the sum of the voltagesaround a closed loop must be zero (they must cancel each other out KVL still applies!)
For the circuit on the previous page:
KVL: -V S + V 1 + V 2 =0 so V S = V 1 + V 2
These voltages have the same signs as the source voltage
KVL: -V S + V X + V Y =0 so V S = -V X - V Y
These voltages have the signs opposite the source voltage
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Example: Voltage Division
RX
R Z
v
X
+v s
3 R R R
Rvv
Z X
X s
X
+
R4 R 5
R 3
Resistors in Series indicates voltage division.
Do NOT include R 4 and R 5 which arent inseriesnot part of the divider, they also havevoltage v S
Find VX
v S
+
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Example: Double Voltage Divider
VS
R 1
R 234 +
- V 2
FIND V 4
First assign element voltages V 2 and V 3 as shown in blue in themiddle diagram.
We will first find an expression for V 2 in terms of V S, and thenwe will find an expression for V 4 in terms of V 2 which we willthen combine.
To find our first expression, we combine resistances obtain thelast circuit where we apply voltage division:
)//(432234
R R R R
S V R R R
V 123 4
23 42
Returning to the middle circuit:
234
44 V R R
RV
Substituting we get our double divider:
S V R R R R R R R
R R R
V 1432
432
34
44 )]//([
)//(
+
- V 4 VS
R 1
R 2
R 3
R 4
+
- V 2
+- V 3
+
- V 4 VS
R 1
R 2
R 3
R 4
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Example: Numeric Double Voltage DividerFIND V 3
First assign element voltage V 30 as shown in blue in the middlediagram.
We will first find an expression for V 30 in terms of V S, and thenwe will find an expression for V 3 in terms of V 30 which we willthen combine.
To find our first expression, we combine resistances obtain thelast circuit where we apply voltage division:
5.7)532//(30 NEW
R
V V V 30405.25.7
5.730
Returning to the middle circuit we write another voltage
division equation where we substitute :
V V V V 9)30(103
5233
303
+
-
V 3
40 V
2.5
30
5
3
2
+
-
V 3
40 V
2.5
30
5
3
2
+
- V 30
40 V
2.5
7.5
+
- V 30
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Review: Current Divider
I s R
2 R 1
I 1 I
2
21
11
11
1
R R
R I I S
Consider tworesistors in parallel that divide current I S:
21
21 R R
R I I S
Current divider presented last week: Equivalent to:
WHY?
Multiply fraction by R 1R 2:
21
2
2
21
1
21
1
21
21
21
211
1
*11
*1
R R R
I
R
R R
R
R R R R R
I
R R
R R
R R R I I S S S
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More on Current Divider
R X R 2
I 2
I X
2
2
211
1 R R
R I R R
R I I X
S
X
X S X
I s
Resistors in Parallel indicate currentdivision.
Do NOT include R 1 which isnt in parallel with Isnot part of thedivider
In general DO NOT include
resistors in series with IS
R1
Find IX
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More on Current Divider
R X R 2
I 2
I X
52111
1
R R R
R I I X
X S X
I s
R1
Find IX
R 5
The addition of R 5 tothe circuit
R 5 is in parallel with I Sas well!
I 5
52
55 111
1
R R R
R I I X
S
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Review: Current Divider
R2 R 1
I 1 I
2
V S+
21
21 R R
R I I S
I s
21
12 R R
R I I S
I X I Y
21
2
R R R I I S X
21
1
R R R I I S Y
Pay attention to the orientation
of the element currents withrespect to the source currents.For currents directed oppositethe source, use a negative signin the current divisionequation
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Double Current Divider Example 1
R 2 IS
R 1 R3
I5
R 4 R 5
R2
IS
R1R3'
IyIx
R 2 IS
R 1 R 3
I5
R 4 R 5
Iy
Ix
Original Problem: Find I 5
Disregard R1 since it is in series withthe current source and doesnt dividecurrent. Assigning Currents I x andIy, we can write the first currentdivider:
y I R R
R I
45
55
/1/1
/1
Obtain new resistanceR3 and write thesecond current divider:
)//(' 5433 R R R R
S y I R R R
I 23
3
/1'/1'/1
Finally substituting (2) into (1) we get:
(1) (2)
S I R R R
R R R
I 23
3
45
55 /1'/1
'/1/1/1
/1
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Double Current Divider Example 2
Original Problem: Find i 1 thru i 4
SECOND CURRENT DIVIDERReturning to the original circuit, we can nowutilize the values we just found for ia and ib tofind the currents through each resistor:
FIRST CURRENT DIVIDERFirst combine resistors on the right in parallel, thencombine resistors on the left in parallel:20//30=(20*30)/(20+30)=600/50=1210//40=(10*40)/(10+40)=400/50=8
Define new currents i a and i b and apply current division:
30A
20
3040
10
i1
i2i4
i3
30A
128
ibia
A Aia 18)30(12812
A Aib 12)30(1288
A Aii b 2.7)12(203030
)(2030
301
A Aii b 8.4)12(203020
)(2030
202
A Aii a 4.14)18(401040
)(4010
403
A Aii a 6.3)18(401010
)(4010
104