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Electrical Power Systems

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

Solution:<br />

Equivalent circuit of the system is shown in ig. 11.5.<br />

Using eqns. (i) and (ii)<br />

ig. 11.5: Equivalent circuit of Example 11.6.<br />

|E g | d = V t + jx d .I ...(i)<br />

I =<br />

Vt-V jx<br />

= 11 1 0<br />

|Eg | d = 11 . q j04<br />

.<br />

. q – º<br />

j1<br />

11 . q – 1<br />

j1<br />

+ HG I KJ<br />

\ |E g | d = 1.1 cos q + j 1.1 sin q + 0.4 ´ 1.1 q – 0.4<br />

...(ii)<br />

\ |E g | d = (1.54 cos q – 0.4) + j 1.54 sin q ...(iii)<br />

Maximum steady-state power capabitity (limit) is reached when d = 90º, i.e., real part of<br />

eqn. (iii) is zero. Thus<br />

1.54 cos q – 0.4 = 0<br />

\ q = 74.9º<br />

\ |E g | = 1.54 sin (74.9º) = 1.486 pu.<br />

\<br />

\ P max =<br />

Vt = 1.1 74. 9º<br />

| Eg| V|<br />

=<br />

( x + x)<br />

1486 10 . ´ .<br />

04 . + 1<br />

\ P max = 1.061 pu. Ans.<br />

11.6 EQUAL-AREA CRITERION<br />

d<br />

In the preceding discussions we have indicated that a solution to the swing equation for d (t),<br />

leads to the determination of the stability of a single machine operating as part of a large power

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