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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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fundamental of stator MMF (produced by any type of winding). The MMF created by balanced<br />

sinusoidal currents is in principle no different than that produced by a single winding save that it<br />

is 3/2 larger and it rotates as a traveling wave whereas the per-phase MMF is a pulsating<br />

standing wave. In fact, with some manipulation (involving the removal of the factor 3/2 and<br />

finding that r<br />

) it could be shown that Equation (3.18) is essentially the same as the torque<br />

expression found in Chapter 2 for the simple sinusoidal motor and CFP winding:<br />

T r<br />

p r<br />

( ) N<br />

D Y<br />

B sin(<br />

) i(<br />

t)<br />

.<br />

Finally, Equations (3.18) and (3.19) can be written in terms of rotor-stator flux linkage. From<br />

Appendix C, the peak value of flux linkage of a sinusoidal winding with a sinusoidal rotor flux is<br />

given by Equation (3.20).<br />

<br />

R NeDY Bp<br />

(3.20)<br />

4<br />

Comparing this with c3 in Equation (3.18) (which is defined by Equation 3.19) it is seen that the<br />

torque can be rewritten as Equation (3.21). This version will be encountered in the SV model of<br />

Part III.<br />

3<br />

T RIpsin( )<br />

(3.21)<br />

2<br />

Phasor Diagram and Single-Phase Equivalent (SPE) Circuit<br />

Now that the rotating field and torque production have been discussed the electrical model for a<br />

synchronous machine will be developed in order to complete the standard treatment. Traditional<br />

analysis of the three-phase synchronous machine employs the use of phasors to describe the<br />

electrical circuit using the “single-phase equivalent” (SPE) concept. 19 In SPE a symmetrical<br />

sinusoidal machine is assumed, driven by balanced sinusoidal currents and operating in steadystate.<br />

Thus the machine can be sufficiently analyzed by examining a single phase (typically<br />

phase-A); all similar phase-B or phase-C quantities are thus unnecessary but may be found simply<br />

by adding a –120° or +120° phase shift to the phase-A quantities.<br />

19 Sometimes this is called the “per-phase equivalent” but that usage is avoided here because the threephase<br />

“phase-variable” model can be analyzed on a per-phase basis and that is not the same as SPE.<br />

82

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