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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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composed of three component space vectors corresponding to each phase as shown in Equation<br />

(3.48). 23<br />

Ne Ne j Ne<br />

<br />

j<br />

f iA()1 t i B() t e iC() t e<br />

2<br />

2<br />

2<br />

<br />

<br />

<br />

j j<br />

fA()1 t fB() t e fC() t e<br />

<br />

<br />

<br />

f f f f<br />

(3.48)<br />

A B C<br />

It is clear that the magnitude of each component is proportional to the current in that phase and<br />

that each component acts in the direction of its magnetic axis. This matches the description of the<br />

MMF components given earlier in the chapter: the distribution is fixed in space, has a peak<br />

aligned to the magnetic axis, and has a magnitude that scales with the phase current. The<br />

definition of the MMF and current space vectors does not require the currents to be balanced<br />

sinusoids but for the moment we will consider this case. The instantaneous values of the<br />

component MMF SVs are shown directed along their respective axes in Figure 3.25 for threephase<br />

currents at electrical positions of 0° and 30°. Figure 3.25 corresponds directly to Figure<br />

3.11, and both figures correspond to Figure 3.7 and Figure 3.8.<br />

Figure 3.25 – Instantaneous values of component and total MMF space vectors; (c.f. Figure 3.11).<br />

23 Throughout this report it will be emphasized that the space vector describes the combined action of the<br />

phases. That emphasis cannot be placed on the space vectors associated with each phase and perhaps this<br />

terminology should not be used but it is found throughout the literature so it is adopted here.<br />

100

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