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Induction generator and excitation capacitor

Short answer

Drive the induction motor above synchronous speed; negative slip reverses rotor current and torque, delivering power. For self-excitation, measure the magnetisation curve, then choose capacitor current line intersecting it. For required voltage, C = Im/(2 pi f V0); minimum C = 1/(omega Xm).

Explain how an induction motor can be used as induction generator. Explain the procedure to determine the value of excitation capacitor required for voltage build up in the generator.

Induction motor as induction generator

If a three-phase induction motor connected to the supply is driven by a prime mover above synchronous speed, the slip becomes negative (s<0s<0). The rotor conductors now cut the rotating field faster than the field itself rotates, so the rotor emf and current reverse. The torque opposes the driving torque, and the machine converts mechanical power into electrical power, which it delivers to the supply. It still draws lagging reactive power from the supply (or from capacitors) for magnetisation.

For an isolated (stand-alone) system the reactive power is supplied by capacitors connected across the stator terminals. This is the self-excited induction generator.

Procedure to find the excitation capacitor

  1. Run the machine as a motor at the supply frequency and no load. Measure terminal (phase) voltage VV against magnetising current ImI_m to get the no-load magnetisation curve (V against ImI_m). It is linear at first and then saturates.
  2. A capacitor of capacitance CC per phase draws a current Ic=VXcI_c = \frac{V}{X_c}, with Xc=12πfCX_c = \frac{1}{2\pi f C}. In the V-I plane it is a straight line through the origin with slope XcX_c.
  3. For stable voltage, the capacitor line must cut the magnetisation curve. The intersection point gives the generated voltage.
  4. For a required voltage V0V_0: read ImI_m at V0V_0 from the curve. Then
Xc=V0Im,C=Im2πfV0X_c = \frac{V_0}{I_m}, \qquad C = \frac{I_m}{2\pi f V_0}
  1. Minimum (critical) capacitance: the line tangent to the linear part of the curve has slope XmX_m (unsaturated magnetising reactance), so
Cmin=1ωXm=1ω2Lm,ω=2πfC_{min} = \frac{1}{\omega X_m} = \frac{1}{\omega^2 L_m}, \quad \omega = 2\pi f

If C<CminC < C_{min}, the line does not meet the curve and the voltage does not build up.

 V
 |            /  Xc line (larger C: flatter)
 |        _.-*---- saturation curve
 |     .-'  /
 |   .'   /
 |  / /
 +------------------> Im
   V0 found at crossing

The generated frequency depends on speed: f≈PNr120f \approx \frac{P N_r}{120} less the small slip, so frequency is a little different from that used in the test. Use the frequency of operation in XcX_c.

✓ Answer checked by Claude Opus 5.5 (high effort)

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