The formula
Half-wave: V_dc = V_pk/π ; Full-wave: V_dc = 2V_pk/π ; Ripple: V_r ≈ I_dc / (f_ripple × C)
- V_pk
- peak of the secondary waveform, less diode drops (volts)
- V_dc
- average output without smoothing (volts)
- V_r
- peak-to-peak ripple with a reservoir capacitor (volts)
- PIV
- peak inverse voltage each diode must withstand
Worked example
A 12 V RMS secondary feeding a bridge rectifier.
- V_pk = 12 × √2 = 16.97 V
- A bridge puts two diodes in series: 16.97 − 1.4 = 15.57 V peak
- Unsmoothed average: V_dc = 2 × 16.97 / π = 10.8 V
About 15.6 V peak with a reservoir capacitor, or 10.8 V average without one.
Where you'll use it
Linear power supply design and the standard comparison question between half-wave, full-wave centre-tapped and bridge circuits. A bridge doubles the ripple frequency to 100 Hz on a 50 Hz supply, so it needs half the smoothing capacitance for the same ripple.