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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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imparted by the definition of the inverse transform. This is made clear when an attempt is made to<br />

take the real part of the phasor only to find that it yields a stationary quantity:<br />

Re X Re j<br />

X e X cos .<br />

p p <br />

In contrast, the inverse of the phasor transform is defined as<br />

1<br />

P X Re j jt X e e Re jt X e<br />

p <br />

j t<br />

and it is seen that the e term is appended to the phasor as a part of the definition of the inverse<br />

transform—the phasor does not contain any “frequency” information itself. The trajectory of the<br />

j t<br />

phasor (coupled to e ) is the same as the trajectory of the SV discussed above for the case of<br />

balanced sinusoidal quantities in steady-state. In contrast, the “frequency” information of the SV<br />

is contained in the SV itself. The SV can represent any 0 combination of the instantaneous<br />

phase variables, whether those variables are changing, stationary, or switching between discrete<br />

values. It is the instantaneous nature of the SV (along with its ability to capture each phase’s<br />

contribution) that make it superior to the phasor for dynamic analysis.<br />

142

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