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Home » GATE Study Material » Electrical Engineering » Electrical Elements » Thevenin Equivalents

Thevenin Equivalents

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Thevenin Equivalents

The ideal voltage source and the resistor are connected in the configuration shown above.

Another important feature of the TEC is that is can explain a drooping terminal voltage. That's inherent in the electrical model itself.

We can write equations that describe the behavior of the TEC when it interacts with other components. First, let us define some variables. If we have a load attached to the terminals some load current will flow. We'll define a load current and a terminal voltage for the TEC as shown below.



Now, write the equation for the circuit. Notice that there will be a voltage across the internal resistance if load current flows.

Vt = Vo - RoIL

Using the expression for the terminal voltage, we can get the plot of terminal voltage against load current.

There are several interesting properties of the TEC that make it a useful model.

The first interesting property is that the source, Vo, is the voltage that is measured when no load is attached. That's called the open circuit voltage. If you just attach a voltmeter to the output terminals - and didn't attach anything else, the voltmeter woud read the value of Vo.

Another interesting property is that the there is a definite limit to how much current this source can supply to a load. If we short the terminals - something you can do in your mind, but not often in practice - the current that will flow is given by:

Short circuit current = Vo/Ro= Io.

Notice the interesting relationship between open circuit votlage, Vo, internal resistance, Ro, and the short circuit current, Io. It looks like Ohm's Law but it really isn't! It doesn't relate current through a resistor to voltage across a resistor.


Q1 If you attach a resistor to a source with a TEC, will the voltage drop below the open-circuit voltage or can it rise above the open-circuit voltage?

Finding A Thevenin Equivalent Circuit

The TEC is a useful way of reducing complexity. If you have a complex circuit interacting with other circuits you don't want to look at all of the details of what is taking place inside the complex circuit - at least you don't often want that.

To illustrate some of the power of the TEC we'll get the TEC for a voltage divider.

The voltage divider isn't a very complex circuit, but it is more complex than the TEC. It can be represented with a TEC, and wherever you find a voltage divider you can replace it with the equivalent TEC. We need to establish values and/or formulas for two items in the voltage divider. Basically, we need two of the following:

  • Open Circuit Voltage

  • Internal Resistance

  • Short Circuit Current.

Let us focus on Open Circuit Voltage, shown as Voin the diagram below. We can use the voltage divider formula to compute the open circuit voltage:

So, we are able to compute one of the three quantities mentioned on the previous page.

Next, focus on theShort Circuit Current. Short circuit current, Io is the current that would flow if the output of the circuit is short circuited. We can imagine shorting the Voltage Divider and shorting the TEC. Wires that short them are shown below and the short circuit current, Isc is indicated.

For the TEC you should be able to see quickly that the short circuit current is just

Vo / Ro . For the voltage divider it's not any more difficult. There the short circuit current is just Vs / Rb. We can use both of these observations to compute the internal resistance of the voltage divider TEC.

Calculate the Short Circuit Current.

Io = Vo / Ro

for the TEC model, and

Io = Vs / Rb

for the voltage divider.

Combining we have

Ro = Vo / Io = Vo / (Vs / Rb )

Continuing, we find:

Ro= Vo / (Vs / Rb ) = [ Vs ( Ra/( Rb + Ra))] / (Vs / Rb )

= RaRb /( Rb + Ra)

So, we have the internal resistance, and it looks like the parallel formula. (But it really isn't!)

At this point you can compute both the open circuit voltge and the internal resistance for the voltage divider, so you have a TEC for the voltage divider. You can use that TEC any place you find the voltage divider. It doesn't matter where you find the voltage divider, you can replace it with its TEC, just like you can replace two parallel resistors by their parallel equivalent.


Q2 You have a battery with an open-circuit voltage of 12.6 volts, and an internal resistance of .05 W

. Is there a .05 W

resistor inside the battery?

Norton Equivalent Circuits

In electrical engineering there is a recurring duality. Voltage and current are duals, and where we find one variable appearing in an expression or a theorem, we usually find the other appearing in a dual expression or theorem. The dual of the Thevenin equivalent model is the Norton equivalent model, a sample of which is given in the figure below.

The relation between terminal voltage and load current for this circuit is interesting because it is indistinguishable from that of the Thevenin Circuit, and the two are electrically equivalent. Write KirchHoff's Current Law for the Norton circuit with a load attached. The result is:

Vterminal/Ro + Iload = Io

So, we find:

Vterminal = RoIo - RoIload

If we identify RoIo with the Vo that appears in the Thevenin model, this is, as claimed, equivalent to the Thevenin model.

Note the following relations between the Thevenin and Norton equivalents.

  • The internal resistance, Ro, is the same in both the Thevenin and Norton circuits.

  • Vo = RoIo, where

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