---
title: "Symmetrical angle control: average and RMS output"
subject: "Power Electronics"
chapter: 2
key: "semester_7/power_electronics:symmetrical-angle-control-derive"
source: https://www.bctengineer.com/q/semester_7/power_electronics/symmetrical-angle-control-derive
site: BCT Engineering
---

# Symmetrical angle control: average and RMS output

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

- Asked in: 2073 Chaitra, 8 marks
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_7/power_electronics/symmetrical-angle-control-derive
- Whole chapter: https://www.bctengineer.com/md/semester_7/power_electronics/chapter-2

## Question

Explain the operation of symmetrical angle control method for power factor improvement. Derive the expression for average and RMS value of the output voltage.

## Short answer

Switch conducts symmetrically about voltage peak, from (π−β)/2 to (π+β)/2, making fundamental input current in phase with voltage. Average output is 2Vm/π sin(β/2). RMS output is (Vm/√2)[(β+sinβ)/π]^1/2.

## Answer

**Symmetrical angle control** is a power factor improvement technique for single-phase converters in which a self-commutated switch (GTO, IGBT, power transistor) conducts for an angle $\beta$ placed **symmetrically about the peak** of each half cycle of supply voltage: it is turned ON at $(\pi-\beta)/2$ and OFF at $(\pi+\beta)/2$. The fundamental input current then lies in phase with the voltage (displacement factor = 1).

#### Circuit

```text
              P (+)
        +-------+-------+-------+
        |       |       |       |
       S1      S2       |       |
        |       |      Dm     Load
 a o----+       +--o b  |    (Ia)
        |       |       |       |
       D1      D2       |       |
        |       |       |       |
        +-------+-------+-------+
              N (-)
 S1, S2: forced-commutated switches (GTO/IGBT)
 Dm: freewheeling diode
```

#### Operation (highly inductive load, $i_o = I_a$ constant)
| Interval ($\omega t$) | Conducting | $v_o$ | $i_s$ |
|---|---|---|---|
| $(\pi-\beta)/2$ – $(\pi+\beta)/2$ | S1, D2 | $v_s$ | $+I_a$ |
| $(\pi+\beta)/2$ – $(3\pi-\beta)/2$ | Dm | $0$ | $0$ |
| $(3\pi-\beta)/2$ – $(3\pi+\beta)/2$ | S2, D1 | $-v_s$ | $-I_a$ |
| $(3\pi+\beta)/2$ – $(5\pi-\beta)/2$ | Dm | $0$ | $0$ |

- S1 is turned OFF by a negative gate pulse (forced turn-off), not by the supply; the load current then transfers to Dm.
- The output is a series of "caps" of the sine wave centred at $90^\circ$ and $270^\circ$.

```text
 vo        ___          ___
          |   |        |   |      caps of |vs|, width b
 ---------+---+--------+---+------
 is       +---+
  +Ia     |   |
 ---------+   +--------+   +------
  -Ia                  +---+
      (90-b/2)(90+b/2)(270-b/2)(270+b/2)
```

#### Average output voltage
The output repeats every $\pi$:

$$
\begin{aligned}
V_{dc} &= \frac{1}{\pi}\int_{(\pi-\beta)/2}^{(\pi+\beta)/2}V_m\sin\omega t\,d(\omega t) = \frac{V_m}{\pi}\left[\cos\frac{\pi-\beta}{2} - \cos\frac{\pi+\beta}{2}\right] \\
&= \frac{V_m}{\pi}\left[\sin\frac{\beta}{2} + \sin\frac{\beta}{2}\right] = \frac{2V_m}{\pi}\sin\frac{\beta}{2}
\end{aligned}
$$

$V_{dc}$ varies from $0$ ($\beta = 0$) to $2V_m/\pi$ ($\beta = \pi$).

#### RMS output voltage

$$
\begin{aligned}
V_{rms}^2 &= \frac{1}{\pi}\int_{(\pi-\beta)/2}^{(\pi+\beta)/2}V_m^2\sin^2\omega t\,d(\omega t) = \frac{V_m^2}{2\pi}\left[\omega t - \frac{\sin2\omega t}{2}\right]_{(\pi-\beta)/2}^{(\pi+\beta)/2} \\
&= \frac{V_m^2}{2\pi}\left[\beta - \frac{\sin(\pi+\beta) - \sin(\pi-\beta)}{2}\right] = \frac{V_m^2}{2\pi}\left[\beta + \sin\beta\right]
\end{aligned}
$$

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

#### Power factor
- $I_s = I_a\sqrt{\beta/\pi}$; fundamental $I_{s1} = \frac{2\sqrt2 I_a}{\pi}\sin\frac{\beta}{2}$ with $\phi_1 = 0$.
- $PF = \dfrac{I_{s1}}{I_s} = \dfrac{2\sqrt2\sin(\beta/2)}{\sqrt{\pi\beta}}$; e.g. at $\beta = 90^\circ$, $PF = 0.90$, whereas a full converter giving the same output ($\cos\alpha = 0.707$) has $PF = 0.64$.

## Check yourself

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

1. In symmetrical angle control, when is the switch on?
   A. From 0 to beta
   B. From alpha to pi
   C. From pi - beta to pi
   D. From (pi-beta)/2 to (pi+beta)/2, symmetric about the voltage peak
   Answer: D. The conduction interval of width beta is centred on 90 degrees (and 270 degrees). (Key point: Switching instants)

2. What is the effect on the fundamental input current?
   A. It leads vs by beta/2
   B. It lags vs by beta/2
   C. It is in phase with vs (displacement factor 1)
   D. It lags by beta
   Answer: C. The current pulse is symmetric about the voltage peak, so phi1 = 0. (Key point: Power factor benefit)

3. What is the average output voltage?
   A. (Vm/pi)(1 + cos(beta))
   B. (2Vm/pi) sin(beta/2)
   C. (2Vm/pi) cos(beta/2)
   D. (Vm/pi) sin(beta)
   Answer: B. Integrating Vm sin(wt) over (pi-beta)/2 to (pi+beta)/2 gives (Vm/pi)[2 sin(beta/2)]. (Key point: Average output voltage)

4. How does the load current continue after S1 turns off?
   A. It stops immediately
   B. It flows through S2
   C. It transfers to the freewheeling diode Dm, with vo = 0
   D. It flows back to the source
   Answer: C. S1 is forced off by its gate and the inductive load current moves to Dm. (Key point: Freewheeling and turn-off)

## Related in Power Electronics

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