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Electrical Power Systems

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80 <strong>Electrical</strong> <strong>Power</strong> <strong>Systems</strong><br />

4.3 MODEL O GENERATOR<br />

An elementary two-pole three-phase synchronous generator model is shown in ig. 4.1. The<br />

rotor and stator are made of high permeability iron to achieve a high ratio of flux density to<br />

mmf. igure 4.1 is highly schematic. igure 4.1 shows each phase winding as if it were a single<br />

turn (the coils aa¢, bb¢ and cc¢) coil placed in a single pair of stator slots. Infact, it is a multiturn<br />

coil physically distributed in a number of stator slots. These three coils aa¢, bb¢ and cc¢, displaced<br />

from each other by 120 electrical degrees. The concentrated full-pitch coils shown here may be<br />

considered to represent distributed windings producing sinusoidal mmf waves concentrated on<br />

the magnetic axes of respective phases. When the rotor is excited to produce an air gap flux (f o<br />

per pole) and is rotating at constant angular velocity (w), the flux linkage of the coil varies with<br />

the position of the rotor mmf axis wt. The flux linkage for an N-turn concentrated coil aa¢ will<br />

be maximum at wt = 0 and zero at wt = p/2. The flux linkage with coil a is given as:<br />

l a = Nf o cos (wt) ...(4.1)<br />

ig. 4.1: Elementary two-pole 3-phase synchronous generator.<br />

The voltage induced in the coil aa¢ is given as:<br />

Ea = - d<br />

( )<br />

dt la = Nfow sin (wt)<br />

\ Ea = Emax cos wt -<br />

p<br />

2<br />

HG I KJ<br />

...(4.2)

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