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LC Tank Oscillator

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Recipe #41 — lc tank oscillator

A freely ringing LC tank loses energy and fades. Add an amplifier that returns just enough energy in the correct phase and the ringing can become a sustained oscillator.

LC TANK OSCILLATOR — SUSTAINING THE RINGING LC TANKCL AMPLIFIERadds just enoughenergy each cycle sensepositive feedback at the resonant frequency Without the amplifier: damped ringing. With correct feedback: steady oscillation.
The tank chooses the frequency; the amplifier replaces the losses. A small part of the oscillation is fed back with the correct phase so the active device gives the LC circuit a little energy each cycle.

An oscillator is controlled positive feedback

Too little feedback and the ringing dies out. Enough properly phased feedback and a steady waveform develops. Too much gain can drive the amplifier into clipping and distort the waveform.

Many practical LC oscillators use this same idea

Hartley oscillators use a tapped inductor or two inductive sections. Colpitts oscillators use a capacitive divider. Armstrong oscillators use transformer coupling. Their details differ, but all provide gain plus frequency-selective positive feedback.

This drawing is intentionally a principle diagram, not a complete buildable oscillator. It keeps the new idea visible before adding the bias networks and device-specific details of a Hartley or Colpitts circuit.

Try these yourself

What primarily selects the oscillation frequency here?
The resonant frequency of the LC network sets the preferred oscillation frequency.
Why is an amplifier needed if the LC tank can already ring?
Real losses make free ringing decay. The amplifier supplies replacement energy.
What type of feedback is required for sustained oscillation?
The fed-back signal must reinforce the existing oscillation at the selected frequency.