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European Journal of Scientific Research - EuroJournals

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A Rule-Based Fuzzy Automatic Voltage Regulator for Power System Stability 927<br />

line to a very large network approximated by an infinite bus. The classical third order single–axis<br />

dynamic model <strong>of</strong> the simple machine infinite bus power system shown in fig 3 has the equations as<br />

follows [12,13]<br />

3.1. Mechanical equations<br />

() t = ω()<br />

-ω<br />

0<br />

� δ t<br />

(1)<br />

ω� () t =<br />

D<br />

ω0<br />

( ω()<br />

t -ω0<br />

) − ( Pe<br />

( t)<br />

− Pm<br />

)<br />

H<br />

2H<br />

(2)<br />

The mechanical input power Pm is assumed to be constant in the excitation controller design.<br />

This implies that the governor action is slow enough not to have any significant impact on the machine<br />

dynamics.<br />

3.2. Electrical generator dynamics<br />

′<br />

1<br />

T ′<br />

( )<br />

() t = E () t − E () t<br />

Eq f q<br />

d 0 (3)<br />

3.3. Electrical equations (assumed X ′ d = X q )<br />

q () t = E′<br />

q () t + ( X d − X ′ d ) I () t<br />

′ f () t = K cU<br />

() t<br />

E′<br />

d ()<br />

() t Vs<br />

sinδ<br />

() t<br />

t =<br />

E d<br />

E f<br />

P<br />

I<br />

I<br />

e<br />

d<br />

q<br />

Q<br />

() t<br />

() t<br />

() t<br />

E′<br />

q<br />

=<br />

X ′ ds<br />

−V<br />

s cosδ<br />

t<br />

X ′<br />

() t ()<br />

Vs<br />

sinδ<br />

=<br />

X ′<br />

E′<br />

q<br />

=<br />

ds<br />

ds<br />

() t<br />

() t V cosδ () t<br />

s<br />

X ′<br />

ds<br />

() t = X I () t<br />

′<br />

E ad f<br />

() t = E′<br />

() t − X ′ I () t<br />

2<br />

s<br />

V<br />

−<br />

X ′<br />

[ ( ) ( () ) ] 2<br />

1<br />

2<br />

2<br />

+ X I t<br />

Vt q d d<br />

d q<br />

ds<br />

(11)<br />

More details <strong>of</strong> the modeling can be seen in [14]. The definitions <strong>of</strong> the parameters are as<br />

indicated under symbols and abbreviations.<br />

X = X + X + X<br />

(12)<br />

ds<br />

ds<br />

d<br />

d<br />

T<br />

T<br />

L<br />

L<br />

X ′ = X ′ + X + X<br />

(13)<br />

X =<br />

X + X<br />

s<br />

T<br />

L<br />

(4)<br />

(5)<br />

(6)<br />

(7)<br />

(8)<br />

(9)<br />

(10)

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