Source and output voltage
VThe bridge keeps the output polarity positive while the source changes sign.
Use both half-cycles. Keep the load polarity. Explore the four-diode bridge after the half-wave rectifier. Follow the conducting diode pair, compare R and RL loads, add nonideal diode drops or an opposing DC voltage, and then study capacitor filtering and source-current harmonics.
The bridge reverses the source connection every half-cycle so that load current keeps the same reference direction.
· Io,rms =
The bridge keeps the output polarity positive while the source changes sign.
The load current keeps its direction; the source current changes sign with the conducting bridge pair.
At θ = 225°, predict the signs of v_s, v_o, i_o and i_s, and which diode pair conducts.
Select RL and increase L. Predict what changes strongly and what remains imposed by the bridge.
Enable V_F and compare the output with the half-wave circuit. How many forward drops are in the active bridge path?
Choose R‖C and increase C. Predict the output-ripple frequency and the change in source-current pulses.
| Voltage ripple factor | — |
|---|---|
| Current ripple factor | — |
| Bridge conduction fraction | — |
| Output peak-to-peak ripple | — |
| Total conduction loss | — |
|---|---|
| Conversion efficiency | — |
| Pair peak current | — |
| Per-diode average current | — |
For R/RL/RLE, the bridge delivers a rectified source through two diodes. When current is zero, conduction starts only when the available rectified source exceeds E.
For R‖C, the capacitor charges when the available bridge voltage exceeds its present voltage and otherwise discharges through R. The ideal source and zero source impedance make the charging-current peaks intentionally idealized.
With ideal bridge diodes, source and load active powers agree in steady state.
Each pair conducts on alternate source half-cycles whenever the bridge is supplying the load.
| Mean output power | — |
|---|---|
| Mean source power | — |
| True source power factor | — |
| Source-current RMS | — |
| RMS current | — |
|---|---|
| Ideal-bridge reverse-voltage reference | — |
| Conduction duty | — |
| Loss in each conducting pair | — |
The source current is alternating even though the load current is rectified. Capacitor filtering can strongly increase current distortion.
Bars show RMS values of source-current harmonics relative to the source frequency; DC is reported separately.
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Source reference: v_s = V_m sin(ωt). Positive load current enters the positive output terminal. D1–D2 conduct for positive source polarity; D3–D4 conduct for negative source polarity. All averages are over one source period.
The capacitor-filter model omits E and L. The series-load model omits C. The source has zero internal impedance and zero commutation inductance, so commutation is instantaneous and capacitor charging peaks are idealized.
Diode forward voltage is constant when enabled. Reverse recovery, switching losses, temperature dependence, transformer copper/core loss and source impedance are not modeled.