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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure 2.16 – Components of total flux (cf. Figure 2.15).<br />

This simple analysis is not valid in practice but is good enough to illustrate some key points.<br />

First, notice that the airgap flux due to the magnet is controlled by the properties of both the<br />

magnetic circuit and the magnet—the magnetic circuit loads the magnet to an operating point.<br />

Further modeling or understanding is not necessary but it is useful to understand the general idea<br />

that the airgap flux due to the magnet is set by the magnetic circuit. Examining Figure 2.15 from<br />

a circuit-theory point of view, if the magnet was an ideal flux source ( Rm ) the airgap flux<br />

would be dominated by the “current source” of magnet flux. If the magnet was not magnetized<br />

but the magnet material kept in place ( r 0 =open circuit) the airgap flux would be comprised<br />

of only coil flux. Also examine these two cases in light of Figure 2.16: it is clear that if the<br />

magnet is ideal the coil cannot influence airgap flux, or if the magnet is not magnetized the coil<br />

completely controls the airgap flux. This is an oversimplified analysis but is useful to know that<br />

real motors are somewhere in between these extremes.<br />

Equally importantly, this model can be used to gain a better understanding of flux linkage. Flux<br />

linkage describes the total flux linked by a winding. A winding in a magnetic circuit can be linked<br />

by lines of flux that were produced by a means external to the winding (mutual flux linkage) and<br />

it can also be linked by lines of flux produced by its own current (self flux linkage). Thus, flux<br />

linkage is an expression that describes the total flux linked by the winding and this expression is<br />

written in terms of the winding’s own current and in terms of the variables that describe the<br />

external source(s) of flux. It follows that a winding’s flux linkage expression will take on a form<br />

consistent with the type of magnetic equipment containing the winding. Two familiar examples<br />

are the standard inductor and the transformer. For the inductor, the flux linkage expression<br />

involves only the flux produced by its own current; there is only one term. For the transformer,<br />

the simplest (ideal) flux linkage expression for a winding would contain a term describing the<br />

flux linkage due to that winding’s current and one term for each additional winding of the<br />

transformer. For a brushless permanent magnet motor, the expression for a winding’s flux linkage<br />

will contain the term describing the flux produced by the winding current, a term describing the<br />

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