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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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can always be written directly in any reference frame. Once again, the fact that the rotor-stator<br />

flux linkage in the rotor frame is simply R could have been recognized from the beginning.<br />

R jr R j r R jr<br />

e Li s e <br />

R e<br />

R R R<br />

Li s <br />

R<br />

R R<br />

Li <br />

(3.148)<br />

s R<br />

Thus, Equations (3.147) and (3.148) are simply Equations (3.138) and (3.139) expressed in the<br />

rotor frame. There is some similarity between Equations (3.138) and (3.147) in that each contains<br />

both a resistance multiplied by a current and the derivative of stator flux linkage. However,<br />

R<br />

transformation into the rotor frame introduced a new term, j R<br />

<br />

. Although it is not obvious in<br />

the given form, this term represents a coupling between the d- and q- components of voltage. To<br />

see this, resolve Equations (3.147) and (3.148) into their dq components (in accordance with<br />

Equation 3.106) to yield Equations (3.149) and (3.150).<br />

d<br />

<br />

vd Rid d q<br />

dt<br />

<br />

d<br />

vq Riq q d<br />

dt<br />

L i <br />

<br />

q<br />

Lsiq d s d R<br />

(3.149)<br />

(3.150)<br />

In Equation (3.149) it is clear that the d-component voltage has a q-component of flux linkage<br />

and vice versa. These are speed voltages and they are the coupling mechanism. However,<br />

Equation (3.149) does not follow obviously from Equation (3.147). To see how it was derived,<br />

examine how the imaginary unit is represented in dq form, Equation (3.151), from which<br />

Equation (3.152) follows.<br />

j /2 cos( / 2) sin( / 2) 0 1<br />

j e<br />

sin( / 2) cos( / 2) 1 0<br />

<br />

<br />

<br />

<br />

<br />

0 j<br />

<br />

0<br />

<br />

<br />

This concept is illustrated in Figure 3.42.<br />

(3.151)<br />

(3.152)<br />

148

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