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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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SV. This was done to obtain a similar SV ( y <br />

) that would be 120<br />

away from the phase-A<br />

axis and that interpretation is valid. But now the more-correct explanation can be provided. It was<br />

mentioned that given our choice of conventions the SV must be defined by Equation (3.69).<br />

jj (3.69): x k xA1xBe xC e<br />

<br />

<br />

<br />

Rotating the SV by 120<br />

to obtain the phase-B projection was accomplished by multiply the<br />

<br />

j120 SV by e<br />

j<br />

e <br />

<br />

. Multiplying that factor through the SV definition yields Equation (3.101).<br />

j j j j<br />

x e k <br />

xA1xBe xC e <br />

<br />

e<br />

j j j<br />

x e k xAe xB1xC e<br />

<br />

<br />

(3.101)<br />

In Equation (3.101) we have done nothing to the definition of the complex plane (the Re/Im or<br />

<br />

α/β axes) but it is clear that the phase variable axes have been rotated by 120<br />

; for example, x A<br />

is no longer acting in a direction coincident with the real axis. Using Equation (3.100) it would be<br />

<br />

seen that in obtaining the phase-C projection, the phase axes are rotated another 120<br />

(for a<br />

<br />

total of 240 120<br />

from the original positions). The action of rotating the SV to align with<br />

the real axis is seen clearly below.<br />

j j<br />

<br />

j j j<br />

j j j<br />

xA Re xA1xBe xC e 1<br />

<br />

<br />

xB Re <br />

xA1xBe xC e <br />

e<br />

<br />

xC Re <br />

xA1xBe xC e <br />

e<br />

<br />

1<br />

j j<br />

<br />

j 1<br />

j<br />

<br />

j j<br />

1 <br />

xA Re xA xBe xC e<br />

<br />

<br />

<br />

xB Re <br />

xAe xB xC e<br />

<br />

<br />

xC Re <br />

xAe xBe x C <br />

<br />

<br />

The apparent axes are shown in Figure 3.32 for the projection onto the phase –A, –B, and –C<br />

axes.<br />

128

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