An inverter turns DC into AC by switching. In sinusoidal PWM (SPWM) a sine reference is compared with a triangular carrier; the amplitude modulation ratio ma is the ratio of the sine peak to the carrier peak. In the linear region (ma ≤ 1) the fundamental output voltage is directly proportional to ma, which is how the inverter (or VFD) controls the AC voltage.
| Inverter | Fundamental output (ma ≤ 1) |
|---|---|
| 1φ Half-bridge | V1(peak) = ma·Vdc/2 → V1(rms) = ma·Vdc/(2√2) |
| 1φ Full-bridge | V1(peak) = ma·Vdc → V1(rms) = ma·Vdc/√2 |
| 3φ (line-to-line RMS) | VLL(rms) = ma·(√3/(2√2))·Vdc = 0.612·ma·Vdc |
Above ma = 1 the inverter enters overmodulation; the output keeps rising but no longer linearly, and low-order harmonics appear. The limit is the six-step (square-wave) mode, where the single-phase full bridge reaches (4/π)·Vdc/√2 ≈ 0.90·Vdc RMS and the three-phase line-to-line RMS reaches 0.78·Vdc.
The amplitude modulation ratio ma is the ratio of the peak of the sinusoidal reference to the peak of the triangular carrier in SPWM. It directly scales the fundamental output voltage in the linear region (ma ≤ 1).
In the linear region the fundamental output is proportional to ma. For a single-phase full bridge V1(rms)=ma·Vdc/√2, so doubling ma doubles the output (up to ma=1).
It is 0 ≤ ma ≤ 1. Within this range the output rises linearly with ma and the harmonics stay near the switching frequency, making them easy to filter.
When ma > 1 the reference exceeds the carrier for part of the cycle, so the output stops rising linearly and low-order harmonics appear. It boosts the fundamental beyond the linear limit at the cost of distortion.
The absolute maximum is the six-step (square-wave) mode: for a single-phase full bridge (4/π)·Vdc/√2 ≈ 0.90·Vdc RMS, and for a three-phase inverter 0.78·Vdc line-to-line RMS.
For SPWM the phase peak is ma·Vdc/2. The line-to-line value is √3 times the phase, and RMS divides the peak by √2, giving √3/(2√2)=0.612 times ma·Vdc.
A full bridge applies the whole DC bus across the load and gives twice the output of a half bridge, which only swings between +Vdc/2 and −Vdc/2. Hence the full-bridge fundamental is ma·Vdc/√2 versus ma·Vdc/(2√2).
mf = fcarrier/foutput is the ratio of the switching (carrier) frequency to the output frequency. A high, odd, integer mf pushes harmonics to high frequencies and keeps the waveform symmetric.
Rearrange the formula. For a three-phase inverter, Vdc = VLL(rms)/(0.612·ma). Designers usually pick ma around 0.85–0.95 to leave margin, which sets the required bus voltage.
Yes. Space-vector modulation (SVPWM) uses the bus about 15% more effectively than basic SPWM, reaching a line-to-line RMS of roughly 0.707·Vdc at the edge of the linear region versus 0.612·Vdc for SPWM.
A VFD keeps a constant volts-per-hertz ratio, so as it raises the output frequency it raises ma to raise the voltage, until ma reaches its limit at base speed. Above that, the motor runs in the field-weakening (constant-power) region.
Zero fundamental output. With no reference signal the inverter produces equal positive and negative pulses that average to zero, so no net AC voltage appears at the output.
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