About the Bridge Rectifier
A bridge rectifier converts alternating current (AC) into pulsating direct current (DC) using four diodes arranged in a diamond ("bridge") pattern. Unlike a half-wave rectifier, which throws away half of every AC cycle, a bridge rectifier uses both halves of the waveform, so it is far more efficient and produces a smoother, higher-average output for the same transformer. This calculator converts an AC RMS voltage, diode drop, load resistance, and filter capacitance into the peak output voltage, DC output voltage, load current, and ripple voltage you would measure at the load.
Understanding the formula
The AC input voltage is normally specified as an RMS value, so the peak of that waveform is Vpeak,in = Vrms × √2. In a bridge rectifier, current always passes through two diodes in series (one on each side of the bridge), so the output peak loses two forward-voltage drops: Vpeak,out = Vpeak,in − 2 × Vf. For a full-wave rectified sine feeding a resistive load, the average (DC) output voltage is Vdc = 2 × Vpeak,out / π ≈ 0.637 × Vpeak,out. Dividing that by the load resistance gives the DC load current, Idc = Vdc / Rload. If a filter (smoothing) capacitor is connected across the load, the peak-to-peak ripple voltage is approximated by Vripple = Idc / (2 × f × C), where f is the AC line frequency and the factor of 2 accounts for the bridge recharging the capacitor twice per input cycle.
Working with units
- Enter the AC input as an RMS voltage (the value a multimeter or a transformer's rated secondary voltage normally reports), not a peak value.
- Diode forward drop is typically about 0.7 V per silicon diode and about 0.3 V per Schottky or germanium diode; the calculator uses whatever value you enter for each of the two conducting diodes.
- Filter capacitance is entered in microfarads (µF); the calculator converts it internally to farads for the ripple formula.
Knowing the limits
This calculator uses idealized diode and capacitor models: it assumes matched diodes with a fixed forward drop (not a full diode I-V curve), a purely resistive load, and the standard small-ripple approximation for the filter capacitor, which is most accurate when the ripple is small relative to the DC output. It does not model transformer winding resistance, diode reverse-recovery losses, or surge current at power-up. For precision power-supply design, treat these results as a solid first-pass estimate and verify with a full circuit simulation or bench measurement.