Power electronic devices: switches that waste little
A normal transistor amplifier holds a voltage and a current at the same time, and gets hot. A power-electronic switch is either fully ON (current flows, voltage across it is near zero) or fully OFF (voltage across it, no current). Power lost = voltage × current, so both cases lose very little. That is why converters are efficient (often above 90%).
- Power diode: one-way, no control. ON when forward biased.
- Thyristor (SCR): ON by a small gate pulse, stays ON until current drops to zero. Used in dimmers and large rectifiers.
- Power MOSFET: very fast ON-OFF, for low voltages and high frequency (chargers, computers).
- IGBT: handles high voltage and high current at medium speed (motor drives, trains, solar inverters).
- Power BJT: older, now rarely used.
Power conversion: four jobs
Input power is changed to the form the load needs. There are four basic jobs:
- AC to DC: rectifier (chargers, DC supplies).
- DC to DC: chopper or DC-DC converter (changes DC level, such as a phone battery step-down).
- DC to AC: inverter (UPS, solar, motor drives).
- AC to AC: AC regulator (dimmer) or cycloconverter (changes voltage or frequency).
Efficiency = power out ÷ power in × 100%. The difference is lost as heat, so power electronics often need a heat sink.
Converter circuits
Half-wave rectifier: one diode. Only the positive half passes. Vavg = Vm / π ≈ 0.318 Vm.
Full-wave bridge rectifier: four diodes. Both halves become positive. Vavg = 2Vm / π ≈ 0.637 Vm, and Vrms = Vm / √2. A capacitor across the load smooths the humps into near-steady DC.
Chopper (buck): a switch ON for time ton out of every period T. The duty cycle D = ton / T. Average output Vout = D × Vin. An inductor and capacitor smooth the pulses.
Single-phase inverter: four switches in an H-shape. Switches 1 and 4 ON gives +V; switches 2 and 3 ON gives −V. Alternating them makes a square wave; a filter or finer switching makes it closer to a sine.
Try it: play with the converters
Open the 3D. Press Half and look at the lamp: it shows about 32%. Predict: what will Full show? (About 64%, twice.) Press Chopper. Move ON time to 25%. Predict the lamp, then check it. Then press Inverter and notice the output swings positive and negative.
At home: a table-fan regulator or a dimmer lamp is a power converter. Turn it slowly and see the brightness change smoothly, though the switch is flicking ON and OFF 100 times a second.
Key formulas and definitions
- Half-wave: V_avg = V_m / π; V_rms = V_m / 2
- Full-wave: V_avg = 2 V_m / π; V_rms = V_m / √2
- Duty cycle D = t_on / T
- Chopper (buck): V_out = D × V_in
- Efficiency η = (P_out / P_in) × 100%
Worked examples
1. A half-wave rectifier gets a sine of peak 325 V. Find the average output.
V_avg = V_m / π = 325 / 3.1416 ≈ 103.5 V.
2. The same input goes to a full-wave rectifier. Find V_avg.
V_avg = 2 V_m / π = 650 / 3.1416 ≈ 206.9 V, twice the half-wave value.
3. A chopper has V_in = 48 V and duty cycle 25%. Find V_out.
V_out = D × V_in = 0.25 × 48 = 12 V.
4. A chopper runs from 12 V and must give 9 V. What duty cycle is needed?
D = V_out / V_in = 9 / 12 = 0.75 = 75%.
5. A converter takes 100 W and gives 95 W. Find its efficiency and the heat loss.
η = 95 / 100 = 95%. Heat lost = 100 − 95 = 5 W.
6. A half-wave rectifier with peak 100 V feeds a 50 Ω resistor. Find the average current.
V_avg = 100 / π = 31.8 V. I_avg = 31.8 / 50 ≈ 0.637 A.
Common mistakes
- Using the full-wave formula for a half-wave circuit. Half-wave is V_m / π; full-wave is 2V_m / π.
- Thinking a rectifier gives perfectly steady DC. It gives humps; a capacitor or filter is needed to smooth them.
- Thinking a switching converter wastes the cut-off power as heat. An ideal switch wastes almost nothing, which is why it is efficient.
- Forgetting that duty cycle is a fraction of the period, not of the voltage: V_out = D × V_in.