# 3.7: Equivalent Circuits - Resistors and Sources

- Page ID
- 1748

- Introduction of equivalent circuits, including the function in v-i relation.

We have found that the way to think about circuits is to locate and group parallel and series resistor combinations. Those resistors not involved with variables of interest can be collapsed into a single resistance. This result is known as an **equivalent circuit**: from the viewpoint of a pair of terminals, a group of resistors functions as a single resistor, the resistance of which can usually be found by applying the parallel and series rules.

This result generalizes to include sources in a very interesting and useful way. Let's consider our simple attenuator circuit (Shown in Figure 3.7.1) from the viewpoint of the output terminals. We want to find the **v-i** relation for the output terminal pair, and then find the equivalent circuit for the boxed circuit. To perform this calculation, use the circuit laws and element relations, but do not attach anything to the output terminals. We seek the relation between

\[v=(R_{1}\parallel R_{2})i+\frac{R_{2}}{R_{1}+R_{2}}v_{in} \nonumber \]

If the source were zero, it could be replaced by a short circuit, which would confirm that the circuit does indeed function as a parallel combination of resistors. However, the source's presence means that the circuit is **not** well modeled as a resistor.

## The Thévenin equivalent

If we consider the simple circuit of Figure 3.7.2, we find it has the **v-i** relation at its terminals of

\[v=R_{eq}i+v_{eq} \nonumber \]

Comparing the two **v-i** relations, we find that they have the same form. In this case the **Thévenin equivalent resistance** is:

\[R_{eq}=R_{1}\parallel R_{2} \nonumber \]

and the **Thévenin equivalent source** has voltage:

\[v_{eq}=\frac{R_{2}}{R_{1}+R_{2}}v_{in} \nonumber \]

Thus, from viewpoint of the terminals, you cannot distinguish the two circuits. Because the equivalent circuit has fewer elements, it is easier to analyze and understand than any other alternative.

For **any** circuit containing resistors and sources, the **v-i** relation will be of the form:

\[v=R_{eq}i+v_{eq} \nonumber \]

and the **Thévenin equivalent circuit** for any such circuit is that of Figure 3.7.2. This equivalence applies no matter how many sources or resistors may be present in the circuit. In the example below, we know the circuit's construction and element values, and derive the equivalent source and resistance. Because Thévenin's theorem applies in general, we should be able to make measurements or calculations **only from the terminals** to determine the equivalent circuit.

To be more specific, consider the equivalent circuit in Figure 3.7.2. Let the terminals be open-circuited, which has the effect of setting the current ** i **to zero. Because no current flows through the resistor, the voltage across it is zero (remember, Ohm's Law says that (

**v=**). Consequently, by applying KVL we have that the so-called open-circuit voltage

*i*R**v**equals the Thévenin equivalent voltage. Now consider the situation when we set the terminal voltage to zero (short-circuit it) and measure the resulting current. Referring to the equivalent circuit, the source voltage now appears entirely across the resistor, leaving the short-circuit current to be:

_{oc}\[i_{sc}=-\frac{v_{eq}}{R_{eq}} \nonumber \]

From this property, we can determine the equivalent resistance.

\[v_{eq}=v_{oc}\\ R_{eq}=-\frac{v_{oc}}{i_{sc}} \nonumber \]

Use the open/short-circuit approach to derive the Thévenin equivalent of the circuit shown in the figure below.

**Solution**

\[v_{oc}=\frac{R_{2}}{R_{1}+R_{2}}v_{in}\\ i_{sc}=-\frac{v_{in}}{R_{1}} \nonumber \]

Resistor **R _{2}** is shorted out in this case. Thus

\[v_{eq}=\frac{R_{2}}{R_{1}+R_{2}}v_{in}\\ R_{eq}=\frac{R_{1}R_{2}}{R_{1}+R_{2}} \nonumber \]

For the circuit depicted in the above figure, let's derive its Thévenin equivalent two different ways. Starting with the open/short-circuit approach, let's first find the open-circuit voltage **v _{oc}. **We have a current divider relationship as

**R**is in parallel with the series combination of

_{1}**R**and

_{2}**R**. Thus

_{3}\[v_{oc}=\frac{i_{in}R_{3}R_{1}}{R_{1}+R_{2}+R_{3}} \nonumber \]

When we short-circuit the terminals, no voltage appears across **R _{3}**, and thus no current flows through it. In short,

**R**does not affect the short-circuit current, and can be eliminated. We again have a current divider relationship:

_{3}\[i_{sc}=-\frac{i_{in}R_{1}}{R_{1}+R_{2}} \nonumber \]

Thus, the Thévenin equivalent resistance is

\[\frac{R_{3}(R_{1}+R_{2})}{R_{1}+R_{2}+R_{3}} \nonumber \]

To verify, let's find the equivalent resistance by reaching inside the circuit and setting the current source to zero. Because the current is now zero, we can replace the current source by an open circuit. From the viewpoint of the terminals, resistor **R _{3}** is now in parallel with the series combination of

**R**and

_{1}**R**. Thus

_{2}\[R_{eq}=R_{3}\parallel R_{1}+R_{2} \nonumber \]

and we obtain the same result.

## Equivalent Circuits

As you might expect, equivalent circuits come in two forms: the voltage-source oriented **Thévenin equivalent **and the current-source oriented **Mayer-Norton equivalent** (See Figure 3.7.3). To derive the latter, the **v-i** relation for the Thévenin equivalent can be written as:

\[v=R_{eq}i+v_{eq} \nonumber \]

or

\[i=\frac{v}{R_{eq}}-i_{eq} \nonumber \]

where

\[i_{eq}=\frac{v_{eq}}{R_{eq}} \nonumber \]

is the Mayer-Norton equivalent source. The Mayer-Norton equivalent shown in Figure 3.7.3 can be easily shown to have this **v-i** relation. Note that both variations have the same equivalent resistance. The short-circuit current equals the negative of the Mayer-Norton equivalent source.

Find the Mayer-Norton equivalent circuit for the circuit below.

**Solution**

\[i_{eq}=\frac{R_{1}}{R_{1}+R_{2}}i_{in} \nonumber \]

\[R_{eq}=R_{3}\parallel R_{1}+R_{2} \nonumber \]

Equivalent circuits can be used in two basic ways. The first is to simplify the analysis of a complicated circuit by realizing the **any** portion of a circuit can be described by either a Thévenin or Mayer-Norton equivalent. Which one is used depends on whether what is attached to the terminals is a series configuration (making the Thévenin equivalent the best) or a parallel one (making Mayer-Norton the best).

Another application is modeling. When we buy a flashlight battery, either equivalent circuit can accurately describe it. These models help us understand the limitations of a battery. Since batteries are labeled with a voltage specification, they should serve as voltage sources and the Thévenin equivalent serves as the natural choice. If a load resistance **R _{L }**is placed across its terminals, the voltage output can be found using voltage divider:

\[v=\frac{v_{eq}R_{L}}{R_{L}+R_{eq}} \nonumber \]

If we have a load resistance much larger than the battery's equivalent resistance, then, to a good approximation, the battery does serve as a voltage source. If the load resistance is much smaller, we certainly don't have a voltage source (the output voltage depends directly on the load resistance). Consider now the Mayer-Norton equivalent; the current through the load resistance is given by current divider, and equals:

\[i=\frac{i_{eq}R_{eq}}{R_{L}+R_{eq}} \nonumber \]

For a current that does not vary with the load resistance, this resistance should be much smaller than the equivalent resistance. If the load resistance is comparable to the equivalent resistance, the battery serves **neither** as a voltage source or a current course. Thus, when you buy a battery, you get a voltage source if its equivalent resistance is much **smaller** than the equivalent resistance of the circuit to which you attach it. On the other hand, if you attach it to a circuit having a small equivalent resistance, you bought a current source.

He was an engineer with France's Postes, Télégraphe et Téléphone. In 1883, he published (twice!) a proof of what is now called the Thévenin equivalent while developing ways of teaching electrical engineering concepts at the École Polytechnique. He did not realize that the same result had been published by Hermann Helmholtz, the renowned nineteenth century physicist, thiry years earlier.

After earning his doctorate in physics in 1920, he turned to communications engineering when he joined Siemens & Halske in 1922. In 1926, he published in a German technical journal the Mayer-Norton equivalent. During his interesting career, he rose to lead Siemen's Central Laboratory in 1936, surruptiously leaked to the British all he knew of German warfare capabilities a month after the Nazis invaded Poland, was arrested by the Gestapo in 1943 for listening to BBC radio broadcasts, spent two years in Nazi concentration camps, and went to the United States for four years working for the Air Force and Cornell University before returning to Siemens in 1950. He rose to a position on Siemen's Board of Directors before retiring.

Edward Norton was an electrical engineer who worked at Bell Laboratory from its inception in 1922. In the **same** month when Mayer's paper appeared, Norton wrote in an internal technical memorandum a paragraph describing the current-source equivalent. No evidence suggests Norton knew of Mayer's publication.