Superposition Theorem
• The superposition theorem extends the use of Ohm’s
Law to circuits with multiple sources.
• Statement:- “The current through, or voltage across,
an element in a linear bilateral network equal to the
algebraic sum of the currents or voltages produced
independently by each source.”
• Superposition theorem is very helpful in determining
the voltage across an element or current through a
branch when the circuit contains multiple number of
voltage or current sources.
 In order to apply the superposition theorem to a network,
certain conditions must be met :
• All the components must be linear, for e.g.- the current is
proportional to the applied voltage (for resistors), flux linkage
is proportional to current (in inductors), etc.
• All the components must be bilateral, meaning that the
current is the same amount for opposite polarities of the
source voltage.
• Passive components may be used. These are components
such as resistors, capacitors, and inductors, that do not
amplify or rectify.
• Active components may not be used. Active components
include transistors, semiconductor diodes, and electron
tubes. Such components are never bilateral and seldom
linear.
Procedure for applying Superposition
Theorem
Circuits Containing Only Independent Sources:-
• Consider only one source to be active at a time.
• Remove all other ideal voltage sources by short circuit & all
other ideal current sources by open circuit.
Voltage source
is replaced by a
Short Circuit
Current source is
replaced by a
Open Circuit
• If there are practical sources, replace them by the
combination of ideal source and an internal
resistances.
• After that, short circuit the ideal voltage source &
open circuit the ideal current source..
Example :1
R1
R2
R3
V1 V2
100 W 20 W
10 W
15 V 13 V
R1 R2
R3
V1
100 W 20 W
10 W
15 V
V2 shorted
REQ = 106.7 W, IT = 0.141 A and IR3
= 0.094 A
R1 R2
R3
V1 V2
100 W 20 W
10 W
15 V 13 V
REQ = 29.09 W, IT = 0.447 A and IR3
= 0.406 A
R1 R2
R3
V2
100 W 20 W
10 W
13 V
V1 shorted
Example :1
R1 R2
V1 V2
100 W 20 W15 V 13 V
Adding the currents gives IR3
= 0.5 A
REQ = 106.7 W, IT = 0.141 A and IR3
= 0.094 A
REQ = 29.09 W, IT = 0.447 A and IR3
= 0.406 A
With V2 shorted
With V1 shorted
0.094 A 0.406 A
Example :1
R1 R2
R3
V1 V2
100 W 20 W
10 W
15 V 13 V
With 0.5 A flowing in R3, the voltage across R3 must
be 5 V (Ohm’s Law). The voltage across R1 must
therefore be 10 volts (KVL) and the voltage across R2
must be 8 volts (KVL). Solving for the currents in R1
and R2 will verify that the solution agrees with KCL.
0.5 A
IR1
= 0.1 A and IR2
= 0.4 A
IR3
= 0.1 A + 0.4 A = 0.5 A
Example :1
Procedure for applying Superposition
Theorem
 Circuits Containing Independent & Dependent
Sources :-
• Consider only one source to be active at a time.
• Remove all other ideal independent voltage sources by
short circuit & all other ideal independent current sources
by open circuit - as per the original procedure of
superposition theorem.
• NEITHER SHORT CIRCUIT NOR OPEN CIRCUIT THE
DEPENDENT SOURCE. LEAVE THEM INTACT AND AS THEY
ARE.
• Dependent Current Source:-
A current source whose parameters are controlled by
voltage/current else where in the system
v = αVx
VDCS
(Voltage Dependent
Current source)
v = βix
CDCS
(Current Dependent
Current source)
• Dependent Voltage Source:-
v = µVx
VDVS
(Voltage Dependent
Voltage source)
v = ρix
CDVS
(Current Dependent
Voltage source)
A voltage source whose parameters are controlled by
voltage/current else where in the system
11
Example :3
Find i0 in the circuit shown below. The circuit involves a dependent source. The
current may be obtained as by using superposition as :
''
0
'
00 iii 
i’
0 is current due to 4A current source
i’’
0 is current due to 20V voltage source
12
To obtain i’
0we short circuit the 20V
sources
i1
i2
i3A.4i1 
0)(152)(3 320
'
212  iiiiii
For loop 2
For loop 1
For loop 3
045)(1)(5 3
'
02313  iiiiii
310 iii' 
For solving i1, i2, i3 A
17
52
i 0
'

13
To obtain i’’
0 , we open circuit the 4A sources
i4
i5
05ii6i ''
054 
For loop 4
052010i- ''
054  ii
For loop 5
A
17
60
i ''
0 
For solving i4 and i5
A
17
8
17
60
17
52
iiiTherefore, ''
0
'
00



5
''
0 ii 
THANK
YOU

Superposition theorem

  • 1.
    Superposition Theorem • Thesuperposition theorem extends the use of Ohm’s Law to circuits with multiple sources. • Statement:- “The current through, or voltage across, an element in a linear bilateral network equal to the algebraic sum of the currents or voltages produced independently by each source.” • Superposition theorem is very helpful in determining the voltage across an element or current through a branch when the circuit contains multiple number of voltage or current sources.
  • 2.
     In orderto apply the superposition theorem to a network, certain conditions must be met : • All the components must be linear, for e.g.- the current is proportional to the applied voltage (for resistors), flux linkage is proportional to current (in inductors), etc. • All the components must be bilateral, meaning that the current is the same amount for opposite polarities of the source voltage. • Passive components may be used. These are components such as resistors, capacitors, and inductors, that do not amplify or rectify. • Active components may not be used. Active components include transistors, semiconductor diodes, and electron tubes. Such components are never bilateral and seldom linear.
  • 3.
    Procedure for applyingSuperposition Theorem Circuits Containing Only Independent Sources:- • Consider only one source to be active at a time. • Remove all other ideal voltage sources by short circuit & all other ideal current sources by open circuit. Voltage source is replaced by a Short Circuit Current source is replaced by a Open Circuit
  • 4.
    • If thereare practical sources, replace them by the combination of ideal source and an internal resistances. • After that, short circuit the ideal voltage source & open circuit the ideal current source..
  • 5.
    Example :1 R1 R2 R3 V1 V2 100W 20 W 10 W 15 V 13 V R1 R2 R3 V1 100 W 20 W 10 W 15 V V2 shorted REQ = 106.7 W, IT = 0.141 A and IR3 = 0.094 A
  • 6.
    R1 R2 R3 V1 V2 100W 20 W 10 W 15 V 13 V REQ = 29.09 W, IT = 0.447 A and IR3 = 0.406 A R1 R2 R3 V2 100 W 20 W 10 W 13 V V1 shorted Example :1
  • 7.
    R1 R2 V1 V2 100W 20 W15 V 13 V Adding the currents gives IR3 = 0.5 A REQ = 106.7 W, IT = 0.141 A and IR3 = 0.094 A REQ = 29.09 W, IT = 0.447 A and IR3 = 0.406 A With V2 shorted With V1 shorted 0.094 A 0.406 A Example :1
  • 8.
    R1 R2 R3 V1 V2 100W 20 W 10 W 15 V 13 V With 0.5 A flowing in R3, the voltage across R3 must be 5 V (Ohm’s Law). The voltage across R1 must therefore be 10 volts (KVL) and the voltage across R2 must be 8 volts (KVL). Solving for the currents in R1 and R2 will verify that the solution agrees with KCL. 0.5 A IR1 = 0.1 A and IR2 = 0.4 A IR3 = 0.1 A + 0.4 A = 0.5 A Example :1
  • 9.
    Procedure for applyingSuperposition Theorem  Circuits Containing Independent & Dependent Sources :- • Consider only one source to be active at a time. • Remove all other ideal independent voltage sources by short circuit & all other ideal independent current sources by open circuit - as per the original procedure of superposition theorem. • NEITHER SHORT CIRCUIT NOR OPEN CIRCUIT THE DEPENDENT SOURCE. LEAVE THEM INTACT AND AS THEY ARE.
  • 10.
    • Dependent CurrentSource:- A current source whose parameters are controlled by voltage/current else where in the system v = αVx VDCS (Voltage Dependent Current source) v = βix CDCS (Current Dependent Current source) • Dependent Voltage Source:- v = µVx VDVS (Voltage Dependent Voltage source) v = ρix CDVS (Current Dependent Voltage source) A voltage source whose parameters are controlled by voltage/current else where in the system
  • 11.
    11 Example :3 Find i0in the circuit shown below. The circuit involves a dependent source. The current may be obtained as by using superposition as : '' 0 ' 00 iii  i’ 0 is current due to 4A current source i’’ 0 is current due to 20V voltage source
  • 12.
    12 To obtain i’ 0weshort circuit the 20V sources i1 i2 i3A.4i1  0)(152)(3 320 ' 212  iiiiii For loop 2 For loop 1 For loop 3 045)(1)(5 3 ' 02313  iiiiii 310 iii'  For solving i1, i2, i3 A 17 52 i 0 ' 
  • 13.
    13 To obtain i’’ 0, we open circuit the 4A sources i4 i5 05ii6i '' 054  For loop 4 052010i- '' 054  ii For loop 5 A 17 60 i '' 0  For solving i4 and i5 A 17 8 17 60 17 52 iiiTherefore, '' 0 ' 00    5 '' 0 ii 
  • 14.