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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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The potential discrepancy (p.108) will first be recounted. The real-valued stator MMF<br />

<br />

<br />

i( t)<br />

cos( ) i ( t)<br />

cos( 120<br />

) i ( ) cos( 120<br />

) <br />

N e<br />

( , t)<br />

A<br />

B<br />

t <br />

2<br />

f C<br />

was put into complex form<br />

f , t<br />

Ne<br />

Re<br />

2<br />

j<br />

i e <br />

<br />

<br />

<br />

<br />

<br />

<br />

(A): <br />

and found to be equivalent to the real-valued MMF description found in the beginning of<br />

the chapter<br />

3 N <br />

<br />

2 2 <br />

e<br />

(B): f , t I cost<br />

p<br />

.<br />

Thus, all that had been done was to put the traditional real-valued result into complex<br />

form and check that it was correct. Then the stator MMF SV was derived using only SV<br />

analysis<br />

N e <br />

f i<br />

2 <br />

and when the SV corresponding to balanced sinusoidal currents<br />

3 j t<br />

i Ipe 2<br />

<br />

<br />

was substituted in<br />

3 Ne<br />

j t<br />

f Ie p<br />

2 2<br />

<br />

<br />

<br />

<br />

it was found that when the real part (c.f. Equation A) was taken<br />

f , t Re <br />

f<br />

Ne <br />

Re 2 <br />

<br />

i<br />

3 Ne<br />

<br />

Ipcos<br />

t<br />

2 2 <br />

(C): <br />

the result did not match Equation (B).<br />

First we should ask why Re is present in Equation (A). The reason is that we had an<br />

expression for MMF (Equation 3.53, p.104) which contained the sum of complex conjugates and<br />

an identity (Equation 3.55) was used to eliminate one conjugate. But we have seen that the SV<br />

ˆ j<br />

x Xe <br />

is defined with respect to the phase-A axis (that is, ξ is measured CCW from 0° which<br />

is defined to be coincident with the phase-A axis). When the SV is one that represents balanced<br />

j t<br />

sinusoidal quantities, x (3 / 2) X e <br />

<br />

<br />

, the projection onto the real axis is<br />

p<br />

135

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