---
title: "Single-phase inverter fundamental output voltage"
subject: "Power Electronics"
chapter: 5
key: "semester_7/power_electronics:single-phase-inverter-r-fundamental"
source: https://www.bctengineer.com/q/semester_7/power_electronics/single-phase-inverter-r-fundamental
site: BCT Engineering
---

# Single-phase inverter fundamental output voltage

Power Electronics · Chapter 5: Inverter

- Asked in: 2082 Baishakh, 8 marks
- Video: [Single Phase Full Bridge Inverter (Basics, Circuit, Working, Waveforms & Applications) Explained](https://www.youtube.com/watch?v=-WU3BxOxvII) — Engineering Funda
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_7/power_electronics/single-phase-inverter-r-fundamental
- Whole chapter: https://www.bctengineer.com/md/semester_7/power_electronics/chapter-5

## Question

Explain the operation of a single-phase inverter with resistive load and derive the expression for fundamental component of the output voltage.

## Short answer

A single-phase full-bridge inverter with resistive load alternates between +Vs (S1,S2 ON) and -Vs (S3,S4 ON) each half cycle, producing a square wave. Fourier analysis gives odd harmonics only: v0(t) = Σ (4Vs/(nπ)) sin nωt, so peak fundamental V1m = 4Vs/π and RMS V1,rms = 4Vs/(√2 π) = 0.9003 Vs.

## Answer

A single-phase inverter converts dc into ac by alternately connecting the load to the dc source in opposite directions. With a resistive load and square-wave switching, the output is a square wave of amplitude $V_s$ (full bridge) or $V_s/2$ (half bridge), and the current has the same shape.

#### Circuit (full bridge)
```text
     +-------+-----------+
     |       |           |
     |      S1          S3
    Vs       |           |
     |       A---[ R ]---B
     |       |    v0     |
     |      S4          S2
     |       |           |
     +-------+-----------+
```

#### Operation
- **$0 < t < T/2$:** S1 and S2 ON. Point A is at $+V_s$ relative to B: $v_0 = +V_s$, $i_0 = V_s/R$.
- **$T/2 < t < T$:** S3 and S4 ON. $v_0 = -V_s$, $i_0 = -V_s/R$.
- S1–S4 (and S3–S2) of a leg must never be ON together. Output frequency $f = 1/T$ is set by the gating rate.
- With a pure R load the current reverses exactly with the voltage, so the feedback diodes do not conduct.
- **Half bridge:** two switches and a centre-tapped source give $v_0 = \pm V_s/2$.

```text
 v0  +Vs |________
         |        |
       0 |--------+--------- t
         |        |________
     -Vs  S1,S2 ON  S3,S4 ON
         0       T/2       T
```

#### RMS value
$$
V_{0,rms} = \left[\frac{2}{T}\int_0^{T/2}V_s^2\,dt\right]^{1/2} = V_s
$$

#### Fundamental component (Fourier analysis)
The wave is odd with half-wave symmetry, so $a_0 = 0$, $a_n = 0$ and only odd sine terms remain:

$$
\begin{aligned}
b_n &= \frac{2}{\pi}\int_0^{\pi}V_s\sin n\theta\,d\theta = \frac{2V_s}{n\pi}\big[-\cos n\theta\big]_0^{\pi} = \frac{2V_s}{n\pi}(1 - \cos n\pi) \\
b_n &= \frac{4V_s}{n\pi}\ (n\ \text{odd}), \qquad b_n = 0\ (n\ \text{even}) \\
v_0(t) &= \sum_{n=1,3,5,\dots}\frac{4V_s}{n\pi}\sin n\omega t
\end{aligned}
$$

For $n = 1$:

$$
\begin{aligned}
V_{1m} &= \frac{4V_s}{\pi} = 1.273\,V_s \\
V_{1,rms} &= \frac{4V_s}{\sqrt2\,\pi} = 0.9003\,V_s
\end{aligned}
$$

For a half bridge, replace $V_s$ by $V_s/2$: $V_{1m} = 2V_s/\pi$, $V_{1,rms} = 0.45\,V_s$.

Distortion: $THD = \sqrt{V_{rms}^2 - V_1^2}/V_1 = \sqrt{1 - 0.9003^2}/0.9003 = 48.3\%$. Example: $V_s = 220$ V gives $V_{1,rms} = 198.1$ V.

## Check yourself

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

1. In a full-bridge inverter with resistive load, which switches are ON in the first half cycle to give v0 = +Vs?
   A. S1 and S4
   B. S3 and S4
   C. S1 and S2
   D. All four
   Answer: C. S1 and S2 (diagonal pair) connect A to +Vs and B to the return; S1-S4 in the same leg must never be ON together. (Key point: Operation of full bridge)

2. For the square wave of amplitude Vs, what is b_n?
   A. 2Vs/(n pi) for all n
   B. 4Vs/(n pi) for odd n, 0 for even n
   C. Vs/(n pi) for odd n
   D. 4Vs/(n pi) for all n
   Answer: B. b_n = (2Vs/n pi)(1 - cos n pi), which is 4Vs/(n pi) for odd n and zero for even n. (Key point: Fourier coefficient)

3. What is the rms value of the fundamental for a full bridge?
   A. 0.45 Vs
   B. Vs
   C. 1.273 Vs
   D. 0.9003 Vs
   Answer: D. V1,rms = 4Vs/(sqrt2 pi) = 0.9003 Vs; 1.273 Vs is the peak. (Key point: Fundamental rms)

4. How does the fundamental change for a half-bridge inverter?
   A. Vs is replaced by Vs/2, giving V1m = 2Vs/pi
   B. It is doubled
   C. It is unchanged
   D. Only odd harmonics become zero
   Answer: A. The half bridge output is ±Vs/2, so every harmonic amplitude is halved. (Key point: Half bridge)

## Related in Power Electronics

- [Single-phase square-wave inverter rms and fundamental](https://www.bctengineer.com/question.md?key=semester_7%2Fpower_electronics%3Asquare-wave-inverter-rms-fundamental) — Power Electronics, chapter 5
- [Single-phase full-wave inverter with 5 Ω load](https://www.bctengineer.com/question.md?key=semester_7%2Fpower_electronics%3Afull-wave-inverter-5ohm) — Power Electronics, chapter 5
- [180° three-phase inverter and fundamental phase voltage](https://www.bctengineer.com/question.md?key=semester_7%2Fpower_electronics%3Ainverter-180-fundamental-per-phase) — Power Electronics, chapter 5
- [Fundamental and 3rd harmonic of three-phase inverter output](https://www.bctengineer.com/question.md?key=semester_7%2Fpower_electronics%3Ainverter-waveform-vdc-fundamental-third) — Power Electronics, chapter 5
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