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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 />

In general, for a drive system,<br />

J = J + J<br />

(2.61)<br />

m<br />

where: J<br />

m<br />

- motor inertia, J<br />

l<br />

load moments <strong>of</strong> inertia.<br />

l<br />

From equation (2.55) and (2.56) one can write:<br />

and, <strong>with</strong> (2.50),<br />

dΩ m 1 = ( M<br />

e − M<br />

l )<br />

(2.62)<br />

dt J<br />

dΩ m 1 3<br />

∗<br />

= ( pb<br />

Im( Ψ<br />

s<br />

Is<br />

) − Ml<br />

)<br />

(2.63)<br />

dt J 2<br />

Finally, the full mathematical model <strong>of</strong> PM synchronous machine which is used in<br />

simulation studies [Appendices] is described in dq , reference frame as:<br />

dΨ<br />

sd<br />

Usd = Rs Isd + − pbΩmΨ sq<br />

(2.64a)<br />

dt<br />

dΨ<br />

sq<br />

Usq = Rs Isq + + pbΩmΨ sd<br />

(2.64b)<br />

dt<br />

Ψ<br />

sd<br />

= LsdIsd +Ψ<br />

PM<br />

(2.65a)<br />

Ψ<br />

sq<br />

= LsqIsq<br />

(2.65b)<br />

dΩ m 1 = ( M<br />

e − M<br />

l )<br />

(2.66)<br />

dt J<br />

3 ∗ 3<br />

M<br />

e<br />

= pbIm( Ψ<br />

s<br />

Is) = pb( ΨsdIsq −Ψ<br />

sqIsd)<br />

(2.67)<br />

2 2<br />

Based on above equations we can create the block scheme <strong>of</strong> the PMSM machine (Fig.<br />

2.9), where the input signals are the voltage components in dq , reference frame<br />

U , U and the output signal is the mechanical speed <strong>of</strong> the rotor Ω<br />

m<br />

. As the external<br />

sd<br />

sq<br />

load torque<br />

M<br />

l<br />

is disturbance.<br />

23

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