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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Trapezoidal and Sinusoidal BPMS Motors<br />

This chapter has developed the per-phase model of a motor and the previous section described<br />

how three of these can be combined to give the complete model of a three-phase motor. Now that<br />

we have this model, the torque production of three-phase trapezoidal and sinusoidal motors will<br />

be examined. This provides an explanation of each motor’s operation, which facilitates a<br />

discussion of whole-motor torque constants and the ideal type of winding current control<br />

(electronic commutation) required of each motor. Finally, the chapter concludes with a<br />

commentary regarding the differences between the trapezoidal and sinusoidal motor. While that<br />

discussion may not be useful to the general reader the conclusions are crucial to the remainder of<br />

the report.<br />

Torque Production<br />

The per-phase torque functions for the sinusoidal and trapezoidal motor types were shown in<br />

Figure 2.22. The per-phase torque produced as a function of rotor position will match the torque<br />

function in shape when a DC current is forced through the winding. In this case if a hand crank<br />

were attached to the shaft and rotated through one revolution, the operator would have to exert<br />

positive (CCW) torque on the crank from 0°-180°, whereas the operator would have to resist the<br />

force of the crank (by applying negative (CW) torque) from 180°-360° as it seeks to return to the<br />

equilibrium point from which it started (both the 0° and 180° positions are equilibrium points).<br />

The force would vary with position according to Figure 2.22, depending on the type of motor.<br />

The concept of a torque function is an important one because it shows this bipolar symmetry that<br />

is present in every PM or wound-field machine. Since the product of bEMF and current divided<br />

by speed is torque, this makes it clear that both DC and AC motors require the polarity of the<br />

armature current to reverse each electrical cycle in order to produce always-positive (but not<br />

constant) torque.<br />

In a traditional brush DC motor the torque function of each winding is made to look something<br />

like that of the trapezoidal motor. The commutator reverses the current flow in each armature<br />

winding every 180°. There are several armature windings, so as one winding is energized another<br />

is de-energized, thereby producing a nearly-constant torque. AC motors do not have a brushcommutator<br />

system and therefore require that the terminal current be reversed every half cycle by<br />

electrical or electronic means. For this reason the action of controlling the current relative to the<br />

shaft position in a brushless motor is sometimes called electronic commutation. There are two<br />

51

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