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Three-phase sinusoidal PWM inverter

Short answer

A three-phase SPWM inverter compares three 120°-shifted sinusoidal references with a high-frequency triangular carrier; each leg switches when ref > carrier, producing PWM line voltages. Fundamental line‑to‑line RMS voltage is 0.612·ma·Vdc (ma ≤ 1), enabling variable voltage/frequency control with low harmonics.

Explain the operation of a three phase sinusoidal PWM inverter with neat circuit diagram and associated waveforms.

A three-phase sinusoidal PWM (SPWM) inverter is a six-switch bridge whose switching instants are fixed by comparing three sinusoidal reference waves (120° apart) with a common high-frequency triangular carrier. The output line voltages are pulse trains whose fundamental is sinusoidal and adjustable in both magnitude and frequency.

Circuit

      +----+--------+--------+
      |    |        |        |
 Vdc/2   S1 D1    S3 D3    S5 D5
  ---  |    |        |        |
  O    +-a  +--b     +--c     |
  ---  |    |        |        |
 Vdc/2   S4 D4    S6 D6    S2 D2
      |    |        |        |
      +----+--------+--------+
        a, b, c -> 3-phase load

Each leg (S1–S4, S3–S6, S5–S2) is switched in a complementary way (with a small dead time). Diodes carry reactive current back to the source.

Principle of operation

  1. Three references vra,vrb,vrcv_{ra}, v_{rb}, v_{rc} of amplitude ArA_r and frequency frf_r (desired output frequency), displaced by 120°.
  2. One triangular carrier vcv_c of amplitude AcA_c and frequency fc≫frf_c \gg f_r.
  3. Leg a: if vra>vcv_{ra} > v_c, S1 is ON and vaO=+Vdc/2v_{aO} = +V_{dc}/2; if vra<vcv_{ra} < v_c, S4 is ON and vaO=−Vdc/2v_{aO} = -V_{dc}/2. Legs b and c work the same way with vrbv_{rb}, vrcv_{rc}.
  4. Line voltage vab=vaO−vbOv_{ab} = v_{aO} - v_{bO} takes values +Vdc+V_{dc}, 0, −Vdc-V_{dc}.
 vc /\/\/\/\/\/\/\/\/\/\/\/\/   carrier
 vra  .-''-.          .-''-
     /      \        /       ref a
 ---'--------\------/--------
               '-..-'
 vaO +Vdc/2 |-| |--| |---| |--|
     -Vdc/2 | |_|  |_|   |_|
          (wide pulses near
           +peak of vra)
 vab  +Vdc  |||| ||||
         0 -------------------
      -Vdc         |||| ||||

Key quantities

  • Amplitude modulation index ma=Ar/Acm_a = A_r/A_c. For ma≤1m_a \le 1 (linear range):
V^aO1=maVdc2VL1,rms=322 maVdc=0.612 maVdc\begin{aligned} \hat V_{aO1} &= m_a\frac{V_{dc}}{2} \\ V_{L1,rms} &= \frac{\sqrt3}{2\sqrt2}\,m_a V_{dc} = 0.612\,m_a V_{dc} \end{aligned}
  • Frequency modulation ratio mf=fc/frm_f = f_c/f_r. It is chosen odd and a multiple of 3, so that the three phases have identical waveforms and triplen carrier harmonics cancel in the line voltages.
  • Output frequency is changed by changing frf_r; output voltage by changing mam_a.

Harmonics

  • Harmonics appear as side-bands around mfm_f, 2mf2m_f, 3mf3m_f, … (e.g. mf±2m_f \pm 2, 2mf±12m_f \pm 1).
  • Low-order harmonics are almost absent, so a small filter (or the load inductance itself) gives near-sinusoidal current.
  • Overmodulation (ma>1m_a > 1): output rises less than linearly and low-order harmonics (5th, 7th) appear; at very large mam_a the inverter becomes a six-step (square-wave) inverter.

Advantages, drawback and uses

  • Voltage and frequency control within the inverter (no variable dc link needed).
  • Low harmonic distortion, small filter.
  • Drawback: higher switching losses than six-step operation.
  • Used in variable-speed induction motor drives (V/f control), UPS and grid-tie inverters.

✓ Answer checked by Claude Opus 5.5 (high effort)

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