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Passive AM Crystal Radio

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Recipe #42 — passive am crystal radio

The crystal radio is a beautiful payoff circuit: resonance, diode detection, capacitance, and audio all work together, yet a strong station can sometimes be heard without any battery-powered amplifier.

PASSIVE AM CRYSTAL RADIO ANTENNA L1 TUNING COILC1 VARIABLE D1 DETECTOR HIGH-Z CRYSTAL EARPHONE C2 small RF bypass No battery: antenna energy → tuned circuit → diode envelope detector → earphone
Signal path: the antenna receives many radio frequencies. L1 and C1 resonate near one station. D1 rectifies the selected AM carrier so the slowly varying audio envelope can drive a high-impedance earphone.

Several earlier lessons meet here

LC resonance selects a narrow frequency range. Diode rectification removes one polarity of the RF waveform. Capacitance and the earphone/load help reject the carrier while preserving the much slower audio variation.

Why crystal radio is such a remarkable teaching circuit

A strong local AM station can sometimes be heard with no battery at all. The received radio wave itself supplies the tiny amount of energy delivered to the earphone. Early detectors used mineral crystals; modern demonstrations often use a germanium or Schottky diode because of its low forward voltage.

Antenna, ground, and earphone matter greatly

Because no amplifier supplies extra power, losses are critical. A long antenna, effective RF ground, high-Q coil, low-loss tuning capacitor, sensitive high-impedance earphone, and low-forward-drop detector can make the difference between hearing a station and hearing nothing.

Try these yourself

What selects the desired AM station?
Changing C1 changes the LC resonant frequency, selecting among radio stations.
What does D1 do?
The diode rectifies the RF so the slower audio envelope can be recovered.
Why is a high-impedance earphone preferred?
A crystal set has very little available power, so a high-impedance sensitive transducer preserves more signal.