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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 />

q−<br />

axis<br />

I sq<br />

I s<br />

Ω s<br />

δ I<br />

d<br />

− axis<br />

I sd<br />

Ψ PM<br />

Figure 2.5. Stator current vector in rotor reference frame.<br />

For two current components using trigonometrical rules we can write:<br />

I = I cosδ<br />

(2.54a)<br />

sd<br />

s<br />

I<br />

I = I sinδ<br />

(2.54b)<br />

sq<br />

s<br />

I<br />

Substituting I , I into equation (2.52), the torque expression can be obtain as:<br />

sd<br />

sq<br />

M 3 1<br />

2<br />

e = b[ PM sin I ( q d) sin2 I]<br />

2 p Ψ I s δ −<br />

2<br />

L − L I s δ<br />

(2.55)<br />

<br />

M<br />

es<br />

For given current amplitude the synchronous and reluctances torque varies according to<br />

the sine <strong>of</strong> torque angle δ<br />

I<br />

. The variation <strong>of</strong><br />

M<br />

er<br />

M<br />

es<br />

and M<br />

er<br />

and resultant torque M<br />

e<br />

<strong>with</strong><br />

torque angle are illustrated in Fig. 2.6. The IPMSM parameters used for this calculation<br />

are given in the Appendices.<br />

e [ ] M Nm<br />

M [ ] er<br />

Nm M<br />

es<br />

[ Nm ]<br />

[deg] δ I<br />

Figure 2.6. Variation <strong>of</strong> synchronous torque M es<br />

, reluctance torque M<br />

er<br />

and resultant<br />

torque M as a function <strong>of</strong> torque angle (for rated current amplitude).<br />

e<br />

20

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