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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure 5.3 – Torque control of sinusoidal motor; phase variable form.<br />

The next step is to employ the inverse Clarke transform to change the three-phase sinusoidal<br />

commutation block into an orthogonal two-phase one. This implements a controller in the<br />

stationary reference frame, as shown in Figure 5.4. The references are generated using Equation<br />

(5.3), where the factor of 3/2 comes from the fact that just two windings must produce the same<br />

torque as the previous three. The current reference signals generated are those shown in Figure<br />

5.8-b and Figure 5.8-c.<br />

ref 3 ref<br />

<br />

i I <br />

2<br />

<br />

ref 3 ref<br />

i I <br />

2<br />

Figure 5.4 – Torque control in stationary reference frame.<br />

sin( ) <br />

p r<br />

cos( ) <br />

p r<br />

Although only the stationary reference frame controller operates using the SV directly, both<br />

versions accomplish the control shown in Figure 5.5, where the SVs are given by Equations (5.4)-<br />

(5.5). As the rotor rotates, r increases and the sinusoidal commutator inherently produces three-<br />

phase (or two-phase) values corresponding to a SV with angle /2 to ensure maximum<br />

torque per current. When the current SV is aligned as such, torque is directly proportional to the<br />

peak current.<br />

r<br />

(5.3)<br />

211

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