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Direct Power and Torque Control of AC/DC/AC Converter-Fed ...

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2. Voltage Source <strong>Converter</strong>s – VSC<br />

dI<br />

L<br />

L<br />

dt<br />

dI<br />

L<br />

L<br />

dt<br />

α<br />

β<br />

dU<br />

C<br />

dt<br />

dc<br />

+ RI = U −U<br />

S ,<br />

(2.70)<br />

Lα<br />

Lα<br />

dc<br />

α<br />

+ RI = U −U<br />

S ,<br />

(2.71)<br />

Lβ<br />

β<br />

= ∑ I<br />

S<br />

Lβ<br />

− I<br />

dc<br />

β<br />

3<br />

=<br />

Lk k load<br />

k = α 2<br />

( I S + I S ) − I .<br />

Lα<br />

α<br />

Where, appropriate switching states are expressed as:<br />

S<br />

=<br />

f<br />

⎛<br />

= S<br />

⎝<br />

1<br />

−<br />

3<br />

⎞<br />

Lβ<br />

β<br />

load<br />

( S + S + S ) , S = ( S − S )<br />

(2.72)<br />

α A ⎜ A A B C ⎟ β<br />

B C<br />

(2.73)<br />

⎠<br />

Equations (2.70) - (2.72) can be represented as a block diagram in stationary αβ<br />

coordinates as in Fig. 2. 16.<br />

1<br />

3<br />

U pα<br />

S α<br />

I load<br />

U Lα<br />

+<br />

−<br />

1<br />

sL + R<br />

I Lα<br />

+<br />

+<br />

3<br />

2<br />

+<br />

−<br />

1 U<br />

dc<br />

sC<br />

U Lβ<br />

+<br />

−<br />

1<br />

sL + R<br />

I Lβ<br />

U pβ<br />

S β<br />

Fig. 2. 16. Model <strong>of</strong> a three-phase VSR in stationary αβ coordinates<br />

2.5.4. VSR Model in Synchronously Rotating xy Coordinates<br />

The two-phase model in stationary αβ coordinates (Eqs. (2.70) - (2.72)), can be<br />

transformed into a two-phase model in synchronously rotating xy coordinates using<br />

the appropriate transformation (see Subsection A.2.3.). Therefore, xy model using<br />

the complex space vector notation can be expressed as:<br />

dI<br />

L<br />

dt<br />

Lxy<br />

+ RI<br />

= U −U<br />

S1 + jω<br />

LI<br />

(2.74)<br />

Lxy<br />

Lxy<br />

dc<br />

xy<br />

L<br />

Lxy<br />

30

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