Physics · Ch 9 — Semiconductor Electronics
Transistor as an Oscillator
Transistor as an Oscillator
An electronic oscillator converts DC energy into AC energy of a chosen (usually high) frequency, ranging from a few Hz to several MHz -- unlike an amplifier, an oscillator needs NO external AC input signal at all; its output is entirely SELF-SUSTAINED. Oscillators are broadly sinusoidal (generating a pure sine wave of constant amplitude and frequency) or non-sinusoidal (generating square, ramp/sawtooth or triangular waveforms). Sinusoidal oscillations are further either damped (amplitude decreasing over time, due to resistive energy loss) or undamped (amplitude staying constant). A transistor oscillator circuit combines three parts: a TANK circuit (an inductor L and capacitor C in parallel, which stores energy alternately in L and C to produce natural oscillations of frequency , per the LC-oscillation physics covered in Volume 1's Section 4.9.1), a transistor AMPLIFIER (which amplifies the tank circuit's own signal, using it as the AC input source instead of an external signal), and a FEEDBACK NETWORK (which routes a portion of the amplified output back to the tank circuit, in phase with the existing oscillation, to replace the energy that resistive losses in the tank's real components would otherwise dissipate each cycle -- without this positive feedback the tank circuit's own oscillations would simply damp out). For SUSTAINED oscillation, the Barkhausen conditions must both hold: the total loop phase shift around the amplifier-plus-feedback loop must be or an integer multiple of , and the loop gain must be exactly unity, (where is the amplifier's voltage gain and here is the feedback network's feedback ratio -- the fraction of output fed back to the input -- NOT the transistor current gain of 9.4.3.3). Different tank-circuit designs give different named oscillator circuits -- Hartley, Colpitts, phase-shift and crystal oscillators are named examples -- and oscillators find use generating periodic waveforms, RF carriers, audio tones, digital clock signals, and TV/CRO sweep circuits. …
What this figure shows. Four small voltage-versus-time graphs side by side: (a) a smooth sinusoidal wave, (b) a square wave abruptly alternating between a high and low level, (c) a ramp/sawtooth wave rising linearly then dropping sharply back to its starting level, and (d) a triangular wave rising and falling linearly in a symmetric zig-zag -- together illustrating that a non-sinusoidal oscillator's output can take several different characteristic shapes, in contrast to a sinusoidal oscillator's si …
What this figure shows. Two voltage-versus-time graphs: panel (a) shows a sinusoidal wave whose amplitude visibly shrinks cycle by cycle, decaying towards zero -- 'damped' oscillations, the natural (unassisted) behaviour of a real tank circuit as its resistive losses drain energy each cycle. Panel (b) shows a sinusoidal wave whose amplitude stays exactly constant cycle after cycle -- 'undamped' oscillations, only achievable by continuously replacing the lost energy via positive feedback, exactly the role the feedb …
What this figure shows. Panel (a) is a block diagram: an 'Amplifier' block receives its input from a 'Tank circuit' block (which is also shown receiving a portion of the amplifier's own output voltage back from a 'Feedback Network' block, closing the loop), with the feedback fraction explicitly labelled feeding back into the loop alongside the tank circuit's own signal. Panel (b) zooms into the tank circuit itself: an inductor L and capacitor C connected in parallel, with a load resistor shown drawing off the oscillating output -- the same basic LC parallel combination whose resonant frequency formula $f_0=1/(2\pi\sq …