Lecture 9 Superposition Superposition Theorem (1/2) • In a linear system, the linear responses of linear independent sources can be combined in a linear.
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Transcript Lecture 9 Superposition Superposition Theorem (1/2) • In a linear system, the linear responses of linear independent sources can be combined in a linear.
Lecture 9
Superposition
Superposition Theorem (1/2)
• In a linear system, the linear responses of
linear independent sources can be combined
in a linear manner.
• This allows us to solve circuits with one
independent source at a time and then
combine the solutions.
– If an independent voltage source is not present it
is replaced by a short circuit.
– If an independent current source is not present it
is replaced by an open circuit.
Superposition Theorem (2/2)
• If dependent sources exist, they must remain
in the circuit for each solution.
• Nonlinear responses such as power cannot be
found directly by superposition
• Only voltages and currents can be found by
superposition
Superposition Example 1 (1/4)
20
10 V
a
I1
5
I2
5A
b
Find I1, I2 and Vab by superposition
Superposition Example 1 (2/4)
Step 1: Omit current source.
20
10 V
a
I11
5
I21
b
5A
By Ohm’s law and the
I11 I 21 0.4 A
voltage divider rule:
Vab1 2.0V
Superposition Example 1 (3/4)
Step 2: Omit voltage source.
20
a
I12
5
I22
b
By the current divider
rule and Ohm’s law :
5A
I12 1.0 A
I 22 4.0 A
Vab 2 20V
Superposition Example 1 (4/4)
20
10 V
a
I1
5
I2
5A
b
Combining
steps 1 & 2, we
get:
I1 I11 I12 0.6 A
I 2 I 21 I 22 4.4 A
Vab Vab1 Vab 2 22V
Superposition Example 2 (1/5)
16
16 A
6
Ix
64 V
16 A
Find Ix by superposition
10
Superposition Example 2 (2/5)
16
16 A
6
Ixa
16 A
Activate only the 16 A Current source at the left. Then
use Current Divider Rule:
10 16
I xa
16 A 13 A
6 10 16
10
Superposition Example 2 (3/5)
16
16 A
6
Ixb
16 A
Activate only the 16 A Current source at the right. Then
use Current Divider Rule:
10
I xb
16 A 5 A
6 10 16
10
Superposition Example 2 (4/5)
16
16 A
6
Ixc
64 V
16 A
10
Activate only the 64 V voltage source at the bottom. Then use
Ohm’s Law:
64V
I xc
2 A
6 10 16
Superposition Example 2 (5/5)
16
16 A
6
Ix
64 V
16 A
10
Sum the partial currents due to each of the sources:
I x I xa I xb I xc 13 A 5 A 2 A 6 A