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Emitter Follower
An emitter follower circuit shown in the figure is widely used in AC amplification circuits. The
input and output of the emitter follower are the base and the emitter, respectively, while the
collector is at AC zero, therefore this circuit is also called common-collector circuit.
DC operating point
Solving the second equation, we get :
and
:
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Example
Assume , , find so that the DC operating point is in the middle of
the load line.
Solving for , we get .
AC small-signal equivalent circuit
Voltage gain:
We assume and therefore can be ignored, and have
Now the voltage gain can be found to be:
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As , is smaller than but approximately equal to 1. Note
that , i.e., the output voltage is in phase with the input voltage.
Input resistance:
The input resistance is in parallel with the resistance of the circuit to its right including
the load , which can be found as the ratio of the voltage and the current . But as
we have
and
Comparing this with the input resistance of the common-emitter circuit ,
we see that the emitter follower has much higher input resistance.
Output resistance:
The output resistance is in parallel with the resistance of the circuit to its left including
the source but excluding , which can be found as the ratio of the open-circuit voltage
( ) and the short-circuit current ( ). As the voltage gain of the emitter
follower is close to unity, the open-circuit output voltage is approximately the same as the source
voltage . The short-circuit current can be found as
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Therefore the output resistance is
The overall output resistance can therefore be found to be
Conclusion:
The emitter follower is a circuit with deep negative feedback, i.e., all of its output is fed
back to become part of its input . The fact that this is a negative feedback can be seen by:
Due to this deep negative feedback, the voltage gain of the emitter follower is smaller than unity.
However, the circuit is drastically improved in terms of its input and output resistances. In fact the
emitter follower acts as an impedance transformer with a ratio of , i.e., the input resistance
is times greater than and the output resistance is times smaller
than .
Comparing this with the input resistance and output resistances of the
common-emitter transistor circuit, we see that the emitter follower circuit has very favorable
input/output resistances.
Although the emitter follower does not amplify voltage, due to its high input resistance drawing
little current from the source, and its low output resistance capable of driving heavy load, it is
widely used as both the input and output stages for a multi-stage voltage amplification circuit.