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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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indeed defined such that common-mode components are simply not contained in the PS & NS or<br />

α & β components; there is obviously good reason for defining the transforms this way. There is a<br />

very meaningful graphical understanding of the ZS component that the interested reader can<br />

pursue [106], [105], [62, p.83], [70, p.25] but for brevity it is not presented here. However, a<br />

simplified and insightful result is shown: if the 0 axis is taken to be orthogonal to the α and β<br />

axes, we can draw a three-dimensional vector (although this does not fit our technical definition<br />

of an SV since it only has two components). From the inverter chapter, the eight base SVs of a<br />

180° inverter were projected onto the αβ plane as shown in Figure D.10. The magnitude of each<br />

4<br />

SV is k2 VDC,<br />

which for k 2/3 is equal to<br />

3 DC<br />

<br />

S V .<br />

Figure D.10 – Projection of base SVs of 180° inverter onto AB plane.<br />

If the thee-dimensional vectors were plotted they would be as shown in Figure D.11 ( k 2/3),<br />

where the cross section is that shown in Figure D.10. This shows a graphical interpretation of the<br />

ZS component of the output voltage. (Be aware that in Figure D.11, only 0 S<br />

<br />

, 1 S<br />

<br />

, 4 S<br />

<br />

, and 7 S<br />

<br />

<br />

are in the αγ plane; S2<br />

and S3<br />

are behind the plane in the β direction. The cross-section<br />

S<br />

<br />

but these are omitted for clarity.)<br />

should show a truncated portion of 5 S<br />

<br />

and 6<br />

326

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