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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 6—Asynchronous Generators 6–12<br />

Figure 5: Permanent-magnet generator connected to a resistive load.<br />

It is desirable to maintain the three line currents at about the same value to minimize<br />

torque fluctuations. It is shown in electrical machinery texts that a three-phase generator<br />

will have a constant shaft torque when operated under balanced conditions. A single-phase<br />

generator or an unbalanced three-phase generator has a torque that oscillates at twice the<br />

electrical frequency. This makes the generator noisy and tends to shorten the life of the shaft,<br />

bearings, and couplers. This is one of the primary reasons single-phase motors and generators<br />

are seldom seen in sizes above about 5 kW. The PM generator will have to be built strongly<br />

enough to accept the turbine torque fluctuations, so some imbalance on the generator currents<br />

should not be too harmful to the system, but the imbalance will need to be minimized to keep<br />

the noise level down, if for no other reason.<br />

The electrical output power P e (the power delivered to the load) of the PM generator per<br />

phase is<br />

The magnitude of the current is<br />

P e = I 2 a R a W/phase (12)<br />

|I a | =<br />

|E a |<br />

√<br />

(Rs + R a ) 2 + X 2 s<br />

A (13)<br />

Therefore the output power can be expressed as<br />

E 2<br />

P e =<br />

aR a<br />

(R s + R a ) 2 + Xs<br />

2<br />

The generated voltage E a can be written as<br />

W/phase (14)<br />

E a = k e ω V (15)<br />

This is basically the same equation as Eq. 1. Here the constant k e includes the flux per<br />

pole since the PM generator is a constant flux machine and also includes any constant factor<br />

Wind Energy Systems by Dr. Gary L. Johnson November 21, 2001

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