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

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<strong>Direct</strong> <strong>Torque</strong> <strong>Control</strong> <strong>with</strong> <strong>Space</strong> <strong>Vector</strong> <strong>Modulation</strong><br />

where:<br />

k<br />

s<br />

=<br />

2<br />

3<br />

R<br />

p<br />

= Ψ and Esy = ΩΨs Ψ<br />

s<br />

.<br />

s<br />

b<br />

Ψ , 2<br />

M<br />

e<br />

pb s<br />

Isy<br />

s<br />

3<br />

The above equations show that the<br />

U<br />

sx<br />

component has influence only on the change <strong>of</strong> stator<br />

flux magnitude<br />

Ψ<br />

s<br />

, and the component<br />

Ω<br />

U<br />

sy<br />

– if the term<br />

Ψs s<br />

Ψ is decoupled – can be<br />

used for torque adjustment. Therefore, the flux and torque quantities can be controlled as<br />

shown in Fig. 5.26.<br />

Note, that this <strong>DTC</strong>-<strong>SVM</strong> scheme formally corresponds to the stator flux oriented voltage<br />

source inverter-fed drive induction motor. The block diagram <strong>of</strong> the <strong>DTC</strong>-<strong>SVM</strong> scheme <strong>with</strong><br />

two PI controllers is shown in Fig. 5.26 The dashed line represents the PMSM part [124,125].<br />

Ψ s _ ref<br />

Ψ s<br />

_<br />

R I<br />

s<br />

sx<br />

U sx<br />

R I<br />

s<br />

sx<br />

∫<br />

Ψ s<br />

R I<br />

s<br />

sy<br />

Ω Ψs<br />

⊗<br />

Ω<br />

Ψ<br />

Ψs s<br />

M e _ ref<br />

_<br />

E sy<br />

U sy<br />

1 Isy<br />

R s<br />

3<br />

2<br />

p<br />

b<br />

Ψ<br />

s _ ref<br />

M e<br />

M e<br />

5.3.1 Digital flux control loop<br />

Figure 5.26. Block diagram <strong>of</strong> the scheme presented in Fig. 5.27<br />

Putting the stator x-axis current expression from equation 2.28a under the assumption Ld<br />

= L<br />

q<br />

into equation (5.37) one can obtaines<br />

U<br />

I<br />

sx<br />

Ψs<br />

−ΨPM<br />

cos<br />

= (5.39)<br />

L<br />

s<br />

δ Ψ<br />

Ψs −ΨPM cosδΨ<br />

d Ψs R d Ψ<br />

s s RsΨ<br />

PM<br />

= R ( ) + = Ψ + − cosδΨ<br />

(5.40)<br />

L dt L dt L<br />

sx s s<br />

s s s<br />

Using Laplace transformation to equation 5.40 can be written as:<br />

U<br />

sx<br />

Rs RsΨ<br />

PM<br />

=Ψ<br />

s<br />

( s+ ) − cosδ Ψ<br />

. (5.41)<br />

L L<br />

s<br />

s<br />

89

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