By the end of the section, you will be able to:
- Find the Thévenin equivalent circuit for any linear circuit
- Calculate the maximum power that can be transferred to a load at any point in a circuit, and the value of the load resistance required to draw maximum power
Thévenin’s theorem states that any linear circuit containing several voltage sources and resistors can be simplified to a Thévenin-equivalent circuit with a single voltage source and resistance connected in series with a load. Specifically, the three components connected in series are (see Figure 7.3.1(b)):
- Load resistor, ;
- Thévenin voltage , found by removing from the original circuit and calculating the potential difference from one load connection point to the other (e.g. from to in Figure 7.3.1(a), either across and or across and );
- Thévenin resistance , found by removing from the original circuit and calculating the total equivalent resistance between the two load connection points (e.g. between and in Figure 7.3.1(a), thus as the equivalent resistance of the parallel combination of and , connected in series with ).
Thévenin’s theorem is particularly useful when the load resistance in a circuit is subject to change. When the load’s resistance changes, so does the current it draws and the power transferred to it by the rest of the circuit. In fact, currents everywhere in a circuit will be subject to change whenever a single resistance changes, and the entire circuit would need to be re-analysed to find the new current through and power transferred to a load. Repeating circuit analysis to find the new current through a load every time its resistance changes would be very time-consuming. In contrast, according to Thévenin’s theorem once
are determined for the rest of the circuit, the current through the load is always simply calculated as
from which the voltage drop across, and power transferred to the load are, respectively,
with respect to
. Example 7.3.1 shows the procedure for doing this for the circuit in Figure 7.3.1(a).
Applying Thévenin’s Theorem
for the circuit in Figure 7.3.1(a).
- Find : note that with the circuit open between and there is no current through, and therefore no voltage drop across . Therefore, the potential difference between and must occur in the loop containing and We are free to choose either parallel branch of that loop, as the potential difference across must equal the potential difference across and by the loop rule. Therefore, we will first determine the current in this loop and apply Ohm’s law to find .
- Find : Proceeding from to we encounter a junction where the circuit branches in two directions, towards and . is an ideal voltage source with no resistance, and can therefore be ignored when calculating equivalent resistance. We then encounter another junction where the two branches reconnect, so and are connected in parallel. Proceeding on, we encounter in series with the parallel connection of and , and eventually reach . We will add these resistances using the rules for adding series and parallel resistors.
The current through the loop with
all connected in series is
By Ohm’s law, the voltage across
By our above reasoning, we therefore have
Then, by our above reasoning,
The potential difference from
was calculated as a drop in potential across
as current flows from the positive to the negative terminal of the voltage source
Along the parallel branch (that is, parallel from the perspective of the load connection points
), potential rises at
, then drops across
, travelling in the clockwise direction. By the loop rule, there must be an overall potential rise in the clockwise direction along this branch that equals negative the potential drop in the clockwise direction across
. Thus, between
along the left branch, travelling in the counter-clockwise direction there is also a drop in potential, equal to
It is important to note that perspective matters when treating components as being connected in series or parallel. Here, when determining the current through
in the open circuit, we noted that current flows through a single circuit loop with
all connected in series, and determined the current through
as the potential drop across the series combination of resistors, divided by the equivalent resistance. However, when calculating
we found that from the perspective of the connection points
are connected along parallel branches of the circuit.
The procedure used here to calculate
is the same as that which we apply to more complex circuits. When doing so, it is important to correctly account for voltage rises and drops across between the two load connection points, although to this end we do have freedom of choice in which branch to follow and can always choose the simplest path.
CHECK YOUR UNDERSTANDING 7.3
The circuit is the same as the one from Example 7.3.1, but with
replaced by a short. Determine
in this case.
Maximum Power Transfer Theorem
Thévenin’s theorem finds a useful application in the maximum power transfer theorem, which states that maximum power will be transferred to a load when its resistance is equal to the Thévenin resistance of the network supplying the power. This interesting and highly useful fact is easily proven by taking the derivative of Equation 7.3.3 with respect to
, setting the result equal to
, and solving for the value of
that maximises the function.
Applying Maximum Power Transfer Theorem
What is the maximum amount of power that can be dissipated in
The maximum amount of power that can be dissipated in
is, by the maximum power transfer theorem, the power dissipated when
for the Thévenin equivalent circuit calculated with respect to
To find this, we first determine
replaced by an open circuit, there are two loops: one, passing through
the other, passing through
. We will calculate the current through
using Mesh Analysis techniques developed earlier, then determine
using Ohm’s law. Note that we do not actually need to calculate any other currents, since
the potential difference between
regardless which branch is taken.
, note that with respect to connection points
are all connected in parallel.
the current in the load is
(see Equation 7.3.1), and the power dissipated in
(cf. Equation 7.3.3).
Using the strategies developed in Mesh Analysis, we can write the matrix equations for this network as
are the clockwise mesh currents in the left and right loops, respectively.
(the actual current in
), we apply Cramer’s rule:
The Thévenin-equivalent voltage is therefore
The Thévenin-equivalent resistance is
Finally, the maximum power dissipated in
It is important to be clear that
is the power dissipated in
The general expression for power dissipated in
is given by Equation 7.3.3.
CC licensed content, Original
- Authored by: Daryl Janzen. Provided by: Department of Physics & Engineering Physics, University of Saskatchewan. License: CC BY: Attribution
Introduction to Electricity, Magnetism, and Circuits by Daryl Janzen is licensed under a Creative Commons Attribution 4.0 International License, except where otherwise noted.
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