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DC Network Analysis

Thevenin's Theorem

Thevenin's theorem is a method of circuit analysis that involves reducing a complex circuit to a simple equivalent circuit. Thevenin's theorem is frequently used to make circuit analysis simpler.

Thevenin's theorem is especially useful in analyzing circuits where only one particular resistor in the circuit (called the load) is subject to change. Example:

Example circuit
Example circuit.

Thevenin's theorem states: Any linear electrical circuit can be replaced at terminals A and B by a simple series circuit consisting of an equivalent voltage source Vth and an equivalent resistance Rth.

Note: A linear circuit is an electronic circuit in which the electronic components' values (such as resistance, conductance, capacitance, inductance, gain, etc.) do not change with the level of voltage or current in the circuit.

The equivalent series circuit will provide the same current through a load as would the original circuit. The equivalent voltage Vth is the voltage "seen" between the two terminals (A and B) being considered in the original network with the load resistance removed. The equivalent resistance Rth is the resistance "seen" between the terminals of the original network when all voltage sources of the original circuit are replaced by a short circuit (wire) and all current sources are replaced by an open circuit (break).

Thevenin equivalent circuit
Thevenin equivalent circuit.

The figure below shows the application of Thevenin's theorem to a simple network. When Thevenin's theorem is applied, the current through RL of the figure below (view A) is the same as the current in RL of the figure below (view D).

Transition of a network to resultant Thevenin-equivalent circuit
Transition of a network to resultant Thevenin-equivalent circuit.

It must be pointed out that Thevenin's theorem establishes equivalency for RL only. The current, voltage, and power of RL in the figure above (view D) are therefore the same as in the figure above (view A). The power supplied to the circuit of figure above (view D) by Vth is not the same as the power supplied to the circuit of figure above (view A) by V.

Thevenin's theorem has the effect of removing a portion of a circuit to make the remaining circuitry easier to analyze. Use of Thevenin's theorem is further demonstrated by the following examples.

Example 1:
Find the Thevenin-equivalent circuit of the circuit shown in the figure below.

Example circuit
Example circuit.

Solution:

Calculating the equivalent voltage Vth

Circuit used to calculate Vth
Circuit used to calculate Vth.

Use Kirchhoff's voltage law and Ohm's law to calculate the current I through elements in series (see the figure above):

Current

The voltage between the points A and B can be figured from the voltages V2 and VR2. This is our equivalent voltage Vth in the equivalent circuit:

Voltage

Calculating the equivalent resistance Rth

Replace the voltage sources V1 and V2 with a wire:

Circuit used to calculate Rth
Circuit used to calculate Rth.

The resistance between the points A and B is equal to R1 and R2 in parallel: 0.8 Ω. This is our equivalent resistance Rth in the equivalent circuit:

Final equivalent circuit
Final equivalent circuit.

Example 2:
Find the Thevenin-equivalent circuit of the circuit shown in the figure below.

Example circuit
Example circuit.

Solution:

Calculating the equivalent voltage Vth

Circuit used to calculate Vth
Circuit used to calculate Vth.

The current I through elements in series is equal to I1.

The voltage between the points A and B can be figured from the voltages V2 and VR2. This is our equivalent voltage Vth in the equivalent circuit:

Voltage

Calculating the equivalent resistance Rth

Replace the current source I1 with a break and the voltage source V2 with a wire:

Circuit used to calculate Rth
Circuit used to calculate Rth.

The resistance between the points A and B is equal to R2: 1 Ω. This is our equivalent resistance Rth in the equivalent circuit:

Final equivalent circuit
Final equivalent circuit.



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