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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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As aforementioned a spatial analysis is required, but we can generalize the spatial relationships to<br />

a degree in order to gain an understanding of the basic electrical model. First, this report is only<br />

concerned with non-salient machines and therefore L will not be a function of rotor position. With<br />

this simplification the expression for stator flux linkage becomes Equation (2.21).<br />

L i(<br />

t)<br />

N(<br />

s ) (<br />

r , s )<br />

(2.21)<br />

Second, regardless of the nature of the last two terms (the distributions of stator winding and rotor<br />

flux) their interaction defines a flux linkage that will be a cyclic function of rotor position. From<br />

an electrical standpoint it makes sense to disregard the details of the two distributions and<br />

represent only the resulting flux linkage, which will be denoted by a new variable, R( r)<br />

. This<br />

new variable represents the component of total stator flux linkage that is due to the rotor flux.<br />

Since it is flux linkage due to the magnets it is sometimes called the “magnet flux linkage,” but<br />

this report will use “rotor-stator flux linkage” because the former term sounds as if we are trying<br />

to describe the flux linking the magnet as opposed to the coil. Using this new variable, the<br />

expression for stator flux linkage becomes Equation (2.22). 4<br />

Li ( )<br />

(2.22)<br />

R r<br />

To recapitulate, Equation (2.22) is the flux linkage of a stator winding. It has two components:<br />

flux linkage due to stator self inductance and flux linkage due to the rotor magnets.<br />

Now, to finish the development of the general electrical model the dependence on rotor angle in<br />

R( r)<br />

will be ignored until the next section. In the meantime we will use the generalized stator<br />

flux linkage expression given by Equation (2.23).<br />

Li <br />

(2.23)<br />

R<br />

Faraday’s law can be applied to Equation (2.23) to find an expression for the voltage induced in<br />

the coil, Equation (2.24).<br />

ddi d<br />

R<br />

gt () L (2.24)<br />

dt dt dt<br />

Equation (2.24) suggests that the induced voltage in the winding of a general BPMS motor could<br />

be modeled as an inductor in series with a voltage source, as shown in Figure 2.17. (To<br />

4 Unfortunately, the variable identified here as R<br />

is sometimes referred to as the “rotor flux linkage” or<br />

the “rotor flux” in the popular literature. It is neither, thus these terminologies are incorrect and misleading.<br />

The reader unfamiliar with the distinction may find Appendix A helpful.<br />

33

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