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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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a number of ways to project the SV onto these axes but only the commonly used method is<br />

discussed here. Since the projecting is done in the αβ plane it seems reasonable to find a way to<br />

make the phase-B and phase-C projections equal to the real part of a complex expression; this is<br />

exactly what the common method does.<br />

If CCW rotation is to be defined to match the positive-sequence order (phase-A, phase-B, phase-<br />

C) with increasing ωt, arranging the phase axes as shown in Figure 3.29 forces the space vector to<br />

be defined as Equation (3.69). (There are various other combinations of definitions and<br />

conventions used in the literature; these obviously lead to different SV definitions.)<br />

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

<br />

<br />

A space vector ˆ j<br />

x( t1) Xe <br />

is at the position shown in Figure 3.31-a at some time t1. Its<br />

projection onto the phase-B axis is also shown; the magnitude of the projection is denoted<br />

x ( t ) , where the subscript indicates that it is a projection onto phase-B, not the actual value of<br />

B<br />

1<br />

the phase variable xB ( t 1)<br />

that produced that SV.<br />

Figure 3.31 – SV projection onto phase axes: (a) actual; (b) alternative.<br />

<br />

<br />

( 120 )<br />

At the same instant t1 another SV ( ˆ j <br />

yt1) Xe is shown in Figure 3.31-b that has a<br />

<br />

magnitude equal to that of x( t1)<br />

but an angle that is 120° less. Its projection onto the phase-A<br />

axis is denoted y A(<br />

t1)<br />

. Since the phase axes are 120° apart, the angle between x and the phase-<br />

B axis is the same as that between y and the phase-A axis. Therefore, because x and y have<br />

126

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