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Direct Torque Control with Space Vector Modulation (DTC-SVM) of ...

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Sensorless Speed <strong>Direct</strong> <strong>Torque</strong> <strong>Control</strong> <strong>with</strong> <strong>Space</strong> <strong>Vector</strong> <strong>Modulation</strong> (<strong>DTC</strong>-<strong>SVM</strong>)<br />

The stator current trajectory can be divided in to eight sectors (see Fig. 6.5a).<br />

7π<br />

8<br />

o<br />

157 .5<br />

Sector 4<br />

− +<br />

5π<br />

8<br />

o<br />

112 .5<br />

Sector 3<br />

− −<br />

3π<br />

8<br />

+ −<br />

o<br />

67 .5<br />

Sector 2<br />

I s<br />

o<br />

22.5<br />

π<br />

8<br />

+ +<br />

Sector 5<br />

o<br />

202 .5<br />

9π<br />

8<br />

Sector 6<br />

+ −<br />

o<br />

247 .5<br />

11π<br />

8<br />

− −<br />

Sector 7<br />

− +<br />

o<br />

292 .5<br />

13π<br />

8<br />

+ +<br />

Sector 8<br />

Sector 1<br />

15π<br />

8 π<br />

−<br />

8<br />

o<br />

337 .5<br />

Figure 6.5. Stator current trajectory.<br />

Based on the measured response <strong>of</strong> phase currents in α,<br />

β coordinates, the<br />

( ) sign I s<br />

+ and sign( I s<br />

)<br />

− is calculated from following formulas:<br />

sign( I )<br />

+ = I + I − I<br />

(6.1)<br />

s sα<br />

sβ<br />

s<br />

sign( I )<br />

− = I −I − I<br />

(6.2)<br />

s sα<br />

sβ<br />

s<br />

The possible combinations <strong>of</strong> sign( I s<br />

)<br />

+ and sign( I s<br />

)<br />

− are shown in Fig. 6.6:<br />

Figure 6.6. Possible combination <strong>of</strong> sign( I s<br />

)<br />

+<br />

sign( I s<br />

) + + − −<br />

−<br />

sign( I s<br />

) + − − +<br />

+ and sign( I s<br />

)<br />

− under short pulse supply.<br />

Let us assuming, for example, the case where the sign( I s<br />

)<br />

+ and sign( I s<br />

)<br />

− have positive<br />

π π<br />

sign. The position γ m<br />

exist in the domain <strong>of</strong> − ~ or 7 π 9 π<br />

~ and two estimated<br />

8 8 8 8<br />

position can be obtained.<br />

The mathematical analysis <strong>of</strong> I , I<br />

sα<br />

sβ waveforms leads to following equations:<br />

I = I +∆ I cos 2γ<br />

(6.3)<br />

sα<br />

s s m<br />

125

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