Derive the Transfer Function of the Common Collector Amplifier with Thevenin’s Theorem

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How to Apply Thevenin’s Theorem for Solving Circuits with Dependent Sources

Besides its use to simplify and calculate currents in electrical circuits, Thevenin’s Theorem is also a great tool that we can use to derive transfer functions. This article will illustrate how to derive the small signal transfer function of the Common-Collector Amplifier with bipolar junction transistors (BJTs).

The circuit is shown in Figure 1. It is also called a repeater, so we expect that the calculated transfer function to be close to unity gain.

common_collector_amplifier1

Figure 1


In this figure I noted with VI the DC input bias level at the transistor input and with vi, the AC input signal, which rides on the DC level. We need to derive the small signal transfer function vo/vi.

Let’s first replace the transistor with its small signal equivalent circuit (see Figure 2). This model is valid for small signals, where the transistor transfer function can be considered linear. For large signals, the model is different involving an exponential relation between its input and output signals.

small_signal_common_collector_amplifier1

Figure 2

Thevenin’s Theorem states that networks with voltage and current sources, as well as resistors are electrically equivalent to one single voltage source and one single resistor in series with the source. In order to apply Thevenin’s Theorem, let’s disconnect RE, as in Figure 3. We will calculate the Thevenin equivalent source of this simplified circuit.

small_signal_common_collector_amplifier_31

Figure 3

In Figure 3 I noted the open circuit voltage with voc. The derivation of this voltage is really simple. From Rsource, r&#8719 and voc loop, the voc equation is

image0041 (1)

We have one node equation in this circuit and the algebraic sum of the node currents has to be zero.

image005 (2)

This equation can only be valid if ib is zero. If ib is zero, then

image006 (3)

Next, we need the Thevenin resistance, rth. This is the resistance seen inside the source, as looking from its output. In a previous article, How to Apply Thevenin’s Theorem – Part 1, I calculated the Thevenin resistance by short-circuiting the voltage sources and disconnecting the current sources. That method is valid for circuits with independent sources. This circuit has a dependent source, &#946 ib, which cannot be disconnected. We need another way to calculate rth.

For circuits with dependent sources, rth is calculated by dividing the open circuit voltage, voc, by the short circuit current, isc, at the circuit output. As such, let’s short-circuit the circuit output, as in Figure 4, and calculate isc.

small_signal_common_collector_amplifier_41

Figure 4

image0081 (4)

and the Thevenin resistance is

image0093 (5)

With voc and rth known, we can calculate the transfer function of the circuit in Figure 1. All that’s left is to connect the emitter resistor, RE at the Thevenin source output as in Figure 5.

thevenin_source_5

Figure 5

RE and rth make a voltage divider for voc, so vo is

image011 (6)

Since voc equals vin, the small signal transfer function of the common collector amplifier is

image0121 (7)

Q. E. D.

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The transfer function shows that the gain of the common-collector amplifier is almost one. Indeed, RE (&#946+1) is large compared to Rsource and r&#8719. Mathematically speaking, when RE (&#946+1) tends to infinity, the vo/vi limit is 1, confirming the universal knowledge that the common collector amplifier has a unity gain.

2 thoughts on “Derive the Transfer Function of the Common Collector Amplifier with Thevenin’s Theorem

  1. How would this analysis produce familiar results when there is some collector resistance and the output is taken at the collector in the inverting amplifier arrangement? Thanks.

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