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Electrical Power Systems

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316 <strong>Electrical</strong> <strong>Power</strong> <strong>Systems</strong><br />

ig. 12.11: Block diagram representation of a generating unit with a reheat turbine.<br />

The block diagram of ig. 12.11 is also applicable to a unit with non-reheat turbine.<br />

However, in this case T r = 0.0.<br />

12.12 STATE-SPACE REPRESENTATION<br />

In ig. 12.11, assume Df = x 1, DP g = x 2, DP v = x 3 and DE = x 4.<br />

Differential equations are written by describing each individual block of ig. 12.11 in terms<br />

of state variable. (Note that S is replaced by d<br />

dt )<br />

x·<br />

1 = -1 1<br />

T x<br />

p<br />

x·<br />

2 = -1 2<br />

T x<br />

r<br />

x·<br />

3 = -1 3<br />

T x<br />

t<br />

x· 4 = -1<br />

RT x<br />

g<br />

+ K<br />

T x<br />

p<br />

<br />

HG<br />

p<br />

2 – K p<br />

T<br />

+ 1 K<br />

T T x -<br />

r<br />

+ 1 4<br />

T x<br />

t<br />

1<br />

– 1 4<br />

T x<br />

g<br />

I<br />

p<br />

D P<br />

...(12.12)<br />

L<br />

r<br />

3 +<br />

t KJ K r<br />

t<br />

+ 1<br />

T u<br />

g<br />

Eqns. (12.12) – (12.15) can be written in matrix form:<br />

L<br />

NM<br />

• x1<br />

• x2<br />

• x3<br />

• x4<br />

O<br />

QP<br />

=<br />

L<br />

NM<br />

-1<br />

T<br />

p<br />

0<br />

K<br />

T<br />

p<br />

p<br />

<br />

HG<br />

-1<br />

1 K<br />

-<br />

T T T<br />

r r<br />

0 0<br />

I<br />

KJ<br />

K<br />

T<br />

-1<br />

1<br />

0 0<br />

Tt Tt<br />

-1-1 0 0<br />

RT T<br />

g g<br />

r<br />

t<br />

t<br />

r<br />

O L<br />

QP<br />

NM<br />

x<br />

x<br />

x<br />

x<br />

1<br />

2<br />

3<br />

4<br />

O<br />

QP<br />

+<br />

T x<br />

L<br />

NM<br />

0<br />

0<br />

0<br />

1<br />

T<br />

g<br />

4<br />

O<br />

QP<br />

u +<br />

L<br />

NM<br />

-K<br />

T<br />

0<br />

0<br />

0<br />

p<br />

p<br />

O<br />

QP<br />

DPL ...(12.13)<br />

...(12.14)<br />

...(12.15)<br />

... (12.16)

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