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Electrical Power Systems

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

14. 39 174. 09°<br />

Ic = 796 . 0<br />

134. 23°<br />

´ ° KA<br />

34.33<br />

\ Ic = 3336 . 39. 86°<br />

KA = 3336 39. 86°<br />

KA<br />

The total fault currents to ground, equal to 3 Ia0, flows from ground to neutral through a<br />

combined neutral grounding reactance j0.2 × 0.2 / (0.2 + 0.2) = j0.1W. Therefore, there is a<br />

voltage drop from ground to neutral equal to (3 Ia0 × j0.1), or a potential rise from ground to<br />

neutral given by (– 3Ia0 × j0.1).<br />

3 EaZ2 Potential rise =<br />

´ j 01<br />

ZZ 1 2 + Z0bZ1 + Z2g<br />

b . g<br />

= 3 7.96 0 2.147 62.24<br />

´ °´ °<br />

34.33 134.23°<br />

´ bj01 . g<br />

= 0.1493 18° KV = 149.3 18° Volt Ans.<br />

Example 10.6: Athree phase synchronous generator with solidly grounded neutral is subjected<br />

to a line-to-line fault on phases b and c accompanied by a ground fault on phase a. Assume that<br />

synchronous generator was running on no load. Develop and draw the sequence networks<br />

simulating the above fault condition.<br />

Solution:<br />

ig. 10.15: Circuit diagram of Example 10.6.<br />

There is a line to ground fault on phase a, therefore V a = 0. urther, the phases b and c are<br />

short circuited.

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