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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure C.3 – Sinusoidal winding density.<br />

To derive the ideal sinusoidal winding function, assume that the radial winding density (which is<br />

always nonnegative) is sinusoidal about the stator as shown in Equation (C.1); [26, p.460], [78,<br />

p.37], [42, p.173], [73, p.9.2].<br />

n( ) N sin( )<br />

(C.1)<br />

p<br />

Np is the peak value of this distribution and it clearly must be less than N because the N turns are<br />

distributed around one-half the stator. To determine the value of Np, the winding density can be<br />

integrated over one side of the stator to obtain the total number of windings. Since we stipulate<br />

that there be N total turns, the result is set equal to N.<br />

set <br />

<br />

N N sin( ) d<br />

0<br />

p<br />

N 2N<br />

p<br />

N <br />

N<br />

N p <br />

2<br />

cos( ) <br />

p<br />

<br />

0<br />

Therefore the winding density is given by Equation (C.2). The density is negative from π to 2π<br />

and this may be interpreted as indicating that the direction of the winding on that side of the stator<br />

is opposite that of the top [42, p.173]. 45<br />

N <br />

n( ) sin(<br />

)<br />

2 <br />

(C.2)<br />

45 The reader is alerted to a conflict in the literature for which the author has no explanation. The majority<br />

of references surveyed agree with the MMF expression given here. However, there are several authoritative<br />

references whose expression lacks the factor ½, such as [87] and [36].<br />

283

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