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

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Modeling and control modes <strong>of</strong> PM synchronous motor drives<br />

The active power requirement as a function <strong>of</strong> torque is illustrated in Fig. 2.17 for the<br />

different control strategies. It can be seen, that all control strategies require<br />

approximately the same value <strong>of</strong> active power for a given torque. CSF control needs<br />

less active power in the region up to 1.3 pu torque.<br />

The reactive power requirement as a function <strong>of</strong> torque is illustrated in Fig. 2.18. It can<br />

be seen, that CTA control requires the highest value <strong>of</strong> active power for a given torque<br />

and the CSF control lowest.<br />

4<br />

QN<br />

[ pu]<br />

3<br />

2<br />

CTA<br />

MTPA<br />

1<br />

UPF<br />

CSF<br />

0<br />

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2<br />

M [ ] eN<br />

pu<br />

Figure 2.18. Reactive power versus electromagnetic torque under different control strategies.<br />

1.1<br />

1<br />

0.9<br />

UPF<br />

CSF<br />

cosφ<br />

0.8<br />

MTPA<br />

0.7<br />

0.6<br />

CTA<br />

0.5<br />

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2<br />

M [ ] eN<br />

pu<br />

Figure 2.19. Power factor as a function <strong>of</strong> electromagnetic torque under different control<br />

strategies.<br />

The power factor as a function <strong>of</strong> torque is illustrated in Fig. 2.19. It can be seen, that as<br />

it could be expected, UPF control requires constant power factor for a given torque.<br />

CSF control is very close to the unity power factor up to 1 pu torque.<br />

The above analysis can be summarized as shown in Table. 2.2.<br />

31

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