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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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called the per-phase torque function. As usual, the uppercase K represents a constant and the<br />

lowercase k represents a function.<br />

T ( r )<br />

kt<br />

( r ) K<br />

t sin( r )<br />

(2.33)<br />

i(<br />

t)<br />

Equation (2.33) is plotted in Figure 2.22; current is held constant. Since it is obvious that the<br />

torque function takes the same shape as the airgap flux density, 6 the torque produced by the<br />

trapezoidal motor is found graphically as shown in the figure. Clearly the polarity of current will<br />

need to match the polarity of the torque function to produce useful torque; this is discussed at the<br />

end of this chapter.<br />

Figure 2.22 – Torque functions of sinusoidal and arbitrary trapezoidal motors.<br />

Expressing torque in terms of the torque function allows easy manipulation of the expression,<br />

even if the torque function is not easily described mathematically. This is demonstrated in<br />

Equation (2.34) and the corresponding simulation diagram is shown in Figure 2.23.<br />

T t r<br />

( t)<br />

k ( ) i(<br />

t)<br />

(2.34)<br />

Figure 2.23 – Simulation diagram for per-phase torque function.<br />

6 To be clear, in this case the torque (a function of rotor position as measured with respect to the stator)<br />

takes on the shape the rotor flux density (a function of the angle about the rotor axis), i.e. replace α with θr.<br />

This is true for the simple concentrated full-pitch winding but is not true in general, as will be discussed<br />

later.<br />

39

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