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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 />

2π<br />

2π<br />

4π<br />

j 1 3<br />

where:1,<br />

3 2<br />

− j j 1 3<br />

a= e =− + j , a = e<br />

3<br />

= e<br />

3<br />

=− − j - complex vectors, 2/3 –<br />

2 2<br />

2 2<br />

normalization factor (guarantee that for balanced sinusoidal waveforms the magnitude<br />

<strong>of</strong> the space vector is equal to the amplitude <strong>of</strong> that phase waveforms).<br />

The elements <strong>of</strong> this space vector satisfy the condition:<br />

KA + KB + KC<br />

= 0<br />

(2.2)<br />

and it means that we have three-phase system <strong>with</strong>out neutral wire.<br />

2.1.1 Voltage and current equations<br />

For idealized motor (Fig. 2.1), the following equations <strong>of</strong> the instantaneous stator phase<br />

voltages can be written [3]:<br />

B<br />

b<br />

Z sB<br />

I sB<br />

a<br />

U sB<br />

S<br />

N<br />

N<br />

S<br />

U sA<br />

γ m<br />

Z sA<br />

A<br />

I sA<br />

I sC<br />

Z sC<br />

U sC<br />

N<br />

S<br />

C<br />

c<br />

Figure 2.1. Layout and symbols for three-phase PMSM electric motor windings.<br />

dΨ<br />

dt<br />

sA<br />

sA<br />

=<br />

sA sA<br />

+ (2.3a)<br />

U I R<br />

U I R<br />

dΨ<br />

dt<br />

sB<br />

sB<br />

=<br />

sB sB<br />

+ (2.3b)<br />

U I R<br />

dΨ<br />

dt<br />

sC<br />

sC<br />

=<br />

sC sC<br />

+ (2.3c)<br />

9

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