---
title: "Full-wave thyristor rectifier, 220 V, 50 Ω, 45°"
subject: "Power Electronics"
chapter: 2
key: "semester_7/power_electronics:full-wave-thyristor-220v-50ohm-45"
source: https://www.bctengineer.com/q/semester_7/power_electronics/full-wave-thyristor-220v-50ohm-45
site: BCT Engineering
---

# Full-wave thyristor rectifier, 220 V, 50 Ω, 45°

Power Electronics · Chapter 2: Single phase AC to DC conversion

- Asked in: 2078 Bhadra, 8 marks
- Video: [Single Phase Full Wave Controlled Rectifier with R Load | Power Electronics | Lecture 43](https://www.youtube.com/watch?v=3CAdY-fnPxA) — Electronics Maddy
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_7/power_electronics/full-wave-thyristor-220v-50ohm-45
- Whole chapter: https://www.bctengineer.com/md/semester_7/power_electronics/chapter-2

## Question

Draw the circuit diagram of single phase full wave rectifier with associated waveforms. A single phase full wave thyristor rectifier has an input voltage of 220V rms. The load is a resistance of 50 ohms and firing angle is 45 degree in each positive half cycle. Find average output voltage, rms output voltage.

## Short answer

For a resistive load, conduction from α to π. Vdc = (Vm/π)(1+cos45°) = 169.06 V. Vrms = (Vm/√2)√[(1/π)(π-α+sin2α/2)] = 209.77 V.

## Answer

A **single-phase full-wave thyristor rectifier** (fully controlled bridge) with a resistive load conducts from $\alpha$ to $\pi$ in each half cycle. With an R load the current becomes zero at $\pi$, so the thyristors turn off naturally and $v_o$ never goes negative.

```text
              P (+)
        +-------+-------+
        |               |
       T1              T3
        |               |
 a o----+               +----o b
        |               |
       T4              T2
        |               |
        +-------+-------+
              N (-)
 ac supply vs between a and b (is into a)
 Load R = 50 ohm between P and N
```

#### Operation and waveforms
- $0 < \omega t < \alpha$: all thyristors OFF, $v_o = 0$.
- $\alpha$ to $\pi$: T1, T2 fired, $v_o = v_s$, $i_o = v_s/R$.
- $\pi$ to $\pi+\alpha$: all OFF, $v_o = 0$.
- $\pi+\alpha$ to $2\pi$: T3, T4 fired, $v_o = -v_s$ (positive).
- The load current has the same shape as $v_o$.

```text
 vs   ___
     /   \             /
 ---/-----\-----------/---
           \___/
 vo     __          __
       |  \        |  \
 ------+---\-------+---\---
 0    45   180   225   360   (deg)
 (chopped half-sine pulses, same for io)
```

#### Expressions

$$
V_{dc} = \frac{1}{\pi}\int_{\alpha}^{\pi} V_m\sin\omega t\, d(\omega t) = \frac{V_m}{\pi}(1+\cos\alpha)
$$

$$
V_{rms} = \frac{V_m}{\sqrt2}\left[\frac{1}{\pi}\left(\pi - \alpha + \frac{\sin2\alpha}{2}\right)\right]^{1/2}
$$

#### Calculation
$V_m = \sqrt2 \times 220 = 311.13$ V, $\alpha = 45^\circ = 0.7854$ rad.

$$
\begin{aligned}
V_{dc} &= \frac{311.13}{\pi}(1 + \cos45^\circ) = 99.04 \times 1.7071 = 169.06\ \text{V} \\
V_{rms} &= 220\left[\frac{1}{\pi}\left(\pi - 0.7854 + \frac{\sin 90^\circ}{2}\right)\right]^{1/2} \\
&= 220\left[\frac{2.8562}{\pi}\right]^{1/2} = 220 \times 0.9535 = 209.77\ \text{V}
\end{aligned}
$$

Load currents: $I_{dc} = 169.06/50 = 3.38$ A, $I_{rms} = 209.77/50 = 4.20$ A.

**Answer: $V_{dc} = 169.06$ V, $V_{rms} = 209.77$ V.**

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. Why does vo never go negative with a resistive load?
   A. A freewheeling diode is used
   B. Current becomes zero at pi, so thyristors turn off naturally
   C. The supply is rectified first
   D. The gate is turned off
   Answer: B. With R load, io = vs/R falls to zero at pi, turning the thyristors off before the supply reverses. (Key point: Resistive-load behaviour)

2. Which formula gives Vdc for a resistive load?
   A. (2Vm/pi) cos alpha
   B. (Vm/pi)(1 + cos alpha)
   C. (Vm/2pi)(1 + cos alpha)
   D. Vm/pi cos alpha
   Answer: B. Integrating Vm sin wt from alpha to pi over a period of pi gives (Vm/pi)(1 + cos alpha). (Key point: Average voltage formula)

3. What is Vdc for 220 V rms and alpha = 45°?
   A. 209.77 V
   B. 198.07 V
   C. 99.04 V
   D. 169.06 V
   Answer: D. Vm = 311.13 V; (311.13/pi)(1 + 0.7071) = 169.06 V. (Key point: Numerical Vdc)

4. Which gives Vrms?
   A. Vs[(1/pi)(pi - alpha + sin(2 alpha)/2)]^(1/2) = 209.77 V
   B. Vdc/sqrt(2) = 119.5 V
   C. Vs cos alpha = 155.6 V
   D. Vm/2 = 155.6 V
   Answer: A. Vrms = 220 x sqrt(2.8562/pi) = 209.77 V. (Key point: RMS formula)

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