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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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the same order as the PS set (arranged A-C-B in the CCW direction) but rotate in the opposite<br />

direction, as shown in Figure D.2. 52<br />

Figure D.2 – An alternate (but equivalent) interpretation of sequence sets.<br />

The sequence order of some low-order harmonics are summarized in Figure D.3.<br />

Figure D.3 – Sequence order of some low-order harmonics.<br />

The component of MMF that a current harmonic produces in a machine will rotate according to<br />

its sequence. To see this it is not necessary to use SV theory but doing eases understanding. The<br />

SVs corresponding to the harmonics of Equations (D.4)-(D.6) are given by Equations (D.7)-<br />

(D.9), respectively, where k 2/3 has been used to achieve magnitude-invariance (a derivation<br />

is given later in this appendix).<br />

j t<br />

x1 Xe 1<br />

<br />

<br />

<br />

x3 0<br />

j5t x X e<br />

5 5<br />

(D.7)<br />

(D.8)<br />

(D.9)<br />

It is clear that PS harmonics would cause a positive rotation, NS harmonics would cause negative<br />

rotation, and ZS harmonics do not cause any rotation. 53 More importantly the phasor diagrams in<br />

52 In the method of symmetrical components (MSC) all phasors are at the fundamental frequency. These<br />

sets discussed here are similar to those of MSC but since they have different frequencies they are not the<br />

same. Therefore when “PS,” “NS,” and “ZS” are used in this report, they refer to general sets that have PS,<br />

NS, and ZS rotation, not those sets particular to the MSC.<br />

53 There are several simultaneous “reasons” why the third-harmonic SV is zero. First, we cannot force ZS<br />

current into a winding when the neutral is isolated (KCL). Second, even if the neutral were grounded so<br />

311

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