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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 />

2.1.2 Instantaneous power and electromagnetic torque<br />

The three-phase star-connection system <strong>with</strong>out neutral wire is shown in Fig. 2.4. This<br />

is classical configuration for AC motor windings connections.<br />

A<br />

I sA<br />

U sAC<br />

U sAB<br />

B<br />

U sA<br />

Z sC<br />

Z sA<br />

U sAB<br />

Z sB<br />

C<br />

U sBC<br />

I sC<br />

U sC U sB<br />

I sB<br />

Figure 2.4. Three-phase star connection system <strong>with</strong>out neutral wire.<br />

For this configuration the expression for instantaneous active power supplied to load<br />

can be expressed as:<br />

P= UsAIsA+ UsBIsB+ UsCIsC<br />

(2.35)<br />

Introducing space vector definition, after some arrangement and taking into account the<br />

relation: I + I + I = 0, the equation (2.35) can be written as:<br />

sA sB sC<br />

3 ∗<br />

P= Re[ U<br />

sABC<br />

IsABC<br />

]<br />

(2.36)<br />

2<br />

For dq , frame, the equation (2.35) for the active power can be expressed as:<br />

3<br />

P= ( UsdIsd + UsqIsq<br />

)<br />

(2.37)<br />

2<br />

Substituting voltage equation (2.4) into (2.36), and adopting Ω<br />

K<br />

= pbΩmone obtains<br />

3 ∗ d Ψ<br />

[Re(<br />

sABC ∗ ∗<br />

P= RsIsABC IsABC + IsABC − jpbΩmΨ sABCIsABC<br />

)] (2.38)<br />

2<br />

dt<br />

Note that<br />

sABC<br />

sABC<br />

2<br />

s<br />

I I ∗ = I and:<br />

3 2 d Ψ<br />

[ Re(<br />

sABC ∗<br />

∗<br />

P= Rs Is + IsABC ) + Re( −jpbΩmΨ sABC<br />

IsABC<br />

)] (2.39)<br />

2<br />

dt<br />

d ΨsABC<br />

Hence, neglecting the losses in stator resistance R<br />

s<br />

and assuming that = 0 , the<br />

dt<br />

electromagnetic power is expressed:<br />

17

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