Power Electronics & Semiconductors

Half-Wave Silicon Diode Rectifier Simulator

Inspect single-diode AC rectification, 0.7V forward barrier drop, and negative half-cycle blocking on a live dual-trace oscilloscope.

Speed
A single silicon diode passes only the positive half-cycles of the AC sine wave (CH1) to the load resistor (CH2), blocking all negative half-cycles.
● CH1: CH1
● CH2: CH2

Engineering Theory & Mathematical Model

V_avg = (Vp − Vf) / π, V_rms ≈ (Vp − Vf) / 2

The simplest AC-to-DC converter uses a single PN junction diode in series with the load. During positive half-cycles above Vf ≈ 0.65V, the diode is forward-biased and conducts; during negative half-cycles, reverse bias widens the depletion zone, reducing leakage current to nanoamps and clamping load voltage at 0V.

Interactive Lab Procedure

  1. Compare the blue full AC sine wave (CH1) with the amber positive-only rectified pulses (CH2).
  2. Notice the subtle ~0.68V peak difference between CH1 and CH2 caused by the real Shockley diode drop.
  3. Grab a Capacitor from the left palette and wire it in parallel with RL to turn this into a filtered half-wave supply!

Technical FAQ

What is the core governing formula for Half-Wave Silicon Diode Rectifier Simulator?

V_avg = (Vp − Vf) / π, V_rms ≈ (Vp − Vf) / 2 — The simplest AC-to-DC converter uses a single PN junction diode in series with the load. During positive half-cycles above Vf ≈ 0.65V, the diode is forward-biased and conducts; during negative half-cycles, reverse bias widens the depletion zone, reducing leakage current to nanoamps and clamping load voltage at 0V.

Can I modify component values and rewire this circuit live?

Yes! The schematic above runs a live MNA SPICE engine. Click any part to adjust parameters, add or delete wires and components, and click Share URL to save your custom topology.

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