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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 steady state voltage components based on the equations (2.34a) and (2.34b) are:<br />

Usd =−pbΩ mLq Iqs =−pbΩ mLq Is<br />

(2.69a)<br />

U = R I + p Ω Ψ = R I + p Ω Ψ (2.69b)<br />

sq s qs b m PM s s b m PM<br />

The amplitude <strong>of</strong> stator voltage vector can be calculated as:<br />

s<br />

2 2<br />

sd sq<br />

U = U + U<br />

(2.70)<br />

The stator flux vector amplitude can be calculated from equations (2.65a-b) as:<br />

s<br />

2 2<br />

sd sq<br />

Ψ = Ψ +Ψ (2.71)<br />

The active and reactive power and also the power factor can be obtained from equations<br />

(2.41),(2.46), (2.47).<br />

Maximum torque per ampere (MTPA) control<br />

The main idea <strong>of</strong> this control is develop the torque using minimum value <strong>of</strong> stator<br />

current amplitude. In this case the I sd<br />

components is not equal zero, and may cancel the<br />

reluctance torque produced by high saliency ratio. Therefore, this control strategy is<br />

recommended for IPMSM.<br />

q−<br />

axis<br />

I s<br />

I sq<br />

δ >= 90<br />

I<br />

<br />

d<br />

− axis<br />

I sd<br />

Figure 2.12. Current vector I s and permanent magnet flux vector Ψ<br />

PM<br />

for maximum torque<br />

per ampere operation (MTPAC).<br />

In order to obtain the maximum torque per ampere we should solve the derivative <strong>of</strong><br />

torque equations (2.55) in respect to torque angle. Solving for torque angle α and taking<br />

into account that only negative sign should be considered for the solution, we can<br />

calculate torque angle as:<br />

Ψ PM<br />

−1 −1 1 1 2<br />

δ<br />

I<br />

= cos [ − + ( ) ]<br />

4( L −L ) I 2 4( L −L ) I<br />

d q s<br />

d q<br />

s<br />

(2.72)<br />

26

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