Oscillation in a circuit is undesirable if the circuit is an amplifier or part of a control system which needs to be stable without oscillation. However, oscillation is desirable in many applications such as sinusoidal signal generator, carrier signal generation is broadcast transmission (radio and TV), clock signal in digital systems, etc.

An oscillator is a feedback system composed of a forward path with gain and a feedback path with gain :

For the system to oscillate at a certain frequency, the feedback needs to be positive for the frequency to be positively reinforced while passing through the forward path in order to sustain the output with zero input . Specifically, the output and the input of a feedback system are related by

(142) |

There exist many different configurations of oscillators based on a single transistor. Shown below are three typical Colpitts oscillators: common-base (CB, left), common emitter (CE, middle), and common collector (CC, right). All such circuits contain a “tank” LC circuit composed of an inductor in parallel with and in series, with a resonant frequency

where | (143) |

Here are the requirements for these circuits to oscillate:

- an LC tank tuning circuit that generates sinusoidal oscillation at its resonant frequency
- a positive feedback loop that sustains the oscillation.

- CB with the base AC grounded: The collector voltage is the
output, a fraction of which at the middle point between the two
capacitors, “tap point”, is fed-back to the emitter to a positive
feedback loop:
(144) - CE with the emitter AC grounded: The collector voltage is
the output, which is fed-back through the LC tank circuit to the base.
As the tap point is grounded, the sinusoidal voltage across the LC
tank produces opposite voltage polarities at the far ends of
and , i.e.,
and
have opposite phases
and thereby form a positive feedback loop:
(145) - CC with the collector AC grounded: This a voltage follower circuit
in which the emitter voltage is the output that follows the input
voltage . The feedback from the emitter through the LC tank circuit
to the base form a positive feedback loop:
(146)

More specifically, we consider the common-collector circuit as an example. To find out why the circuit oscillates and the resonant frequency, we disconnect the base path of the circuit and consider the open-loop gain of of the feedback loop. We further model the transistor by a Thevenin voltage source in series with an internal , as shown in the figure:

As the load of the Thevenin source, the tank circuit receives an input at the tap point, and produces an output across the parallel combination of and in series with . Applying KCL at the tap point we get:

(147) |

(148) |

(149) |

i.e. | (150) |

(151) |

When , the denominator becomes zeros and , i.e., there is no current drawn from the source by the tank circuit. Consequently, the voltage drop across is zero and the voltage received by the tank circuit is . Now the output voltage can be found by voltage divider:

i.e. | (152) |

(153) |

We see that when , the open-loop gain is real but greater than 1. However, the non-linearity of the transistor as the feedback path (from to ) will force the open-loop to be 1. The circuit is an oscillator with frequency at .