Thévenin's theorem states that any linear two-terminal circuit can be replaced by an equivalent circuit consisting of an ideal voltage source (VTh) in series with a resistor (RTh). VTh is equal to the open-circuit voltage at the terminals and RTh is the equivalent input resistance when independent sources are turned off. To find the Thevenin equivalent circuit, first the load is replaced with an open circuit to find VTh, then independent sources are turned off to find RTh, the resistance seen looking into the terminals. Once the Thevenin equivalent circuit is determined, it can be used to solve for voltages and currents in the original circuit.

1. Topic : Thévenin’s Theorems
Branch : Batch :

2. Name ENROLLMENT NO.
Abhishek Chokshi 140120109005
Himal Desai
Harsh Dedakia
140120109008
140120109012

4.  A linear two-terminal circuit can be replaced with
an equivalent circuit of an ideal voltage source,
VTh, in series with a resistor, RTh.
◦ VTh is equal to the open-circuit voltage at the terminals.
◦ RTh is the equivalent or input resistance when the
independent sources in the linear circuit are turned off.

6. Linear circuit is a circuit where the
voltage is directly proportional to the
current (i.e., Ohm’s Law is followed).
Two terminals are the 2 nodes/2
wires that can make a connection
between the circuit to the load.

7. Open-circuit voltage Voc is the voltage, V, when the load is an open
circuit (i.e., RL = ∞Ω).
+
Voc
_
ThOC VV =

8. Input resistance is the resistance seen by the
load when VTh = 0V.
It is also the resistance of the linear circuit when
the load is a short circuit (RL = 0Ω).
SCThThin iVRR ==

9. 1. Identify the load, which may be a resistor or a part of
the circuit.
2. Replace the load with an open circuit .
3. Calculate VOC. This is VTh.
4. Turn off all independent voltage and currents sources
in the linear 2-terminal circuit.
5. Calculate the equivalent resistance of the circuit.
This is RTh.
 The current through and voltage across the load in series
with VTh and RTh is the load’s actual current and voltage in the
original circuit.

10. Example
=
RTh
voc
Ω=
1
0i
RTh

11. THEVENIN & NORTON
THEVENIN’S THEOREM:
Find VX by first finding VTH and RTH to the left of A-B.
1 2 Ω 4 Ω
6 Ω 2 Ω V X3 0 V +_
+
_
A
B
•
•
Circuit for Example
First remove everything to the right of A-B.

12. THEVENIN & NORTON
THEVENIN’S THEOREM:
1 2 Ω 4 Ω
6 Ω3 0 V +_
A
B
•
•
Circuit for finding VTH for Example
(30)(6)
10
6 12
ABV V= =
+
Notice that there is no current flowing in the 4 Ω resistor
(A-B) is open. Thus there can be no voltage across the
resistor.

13. THEVENIN & NORTON
THEVENIN’S THEOREM:
We now deactivate the sources to the left of A-B and find
the resistance seen looking in these terminals.
1 2 Ω 4 Ω
6 Ω
A
B
•
•
RTH
Circuit for find RTH for Example
We see,
RTH = 12||6 + 4 = 8 Ω

14. THEVENIN & NORTON
THEVENIN’S THEOREM:
After having found the Thevenin circuit, we connect this
to the load in order to find VX.
8 Ω
1 0 VV T H
R T H
2 Ω V X
+
_
+
_
A
B
•
•
after connecting Thevenin
circuit.
10 2
2
2 8
= =
+
( )( )
XV V

15. THEVENIN & NORTON
THEVENIN’S THEOREM:
In some cases it may become tedious to find RTH by reducing
the resistive network with the sources deactivated. Consider
the following:
V T H
R T H
+
_
A
B
•
•
I S S
A Thevenin circuit with the output shorted.
We see;
TH
TH
SS
V
R
I
=

16. circuits
Thevenin