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7/27/2019 TSA8
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7/27/2019 TSA8
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The apparent impedance seen by animpedance relay at C looking towards the
line is given by 0 E E
E Z Z
I ~
I ~
Z E ~
I ~
E ~
Z
B A
AT A
AAC C
∠∠∠∠−
−−−∠
∠∠∠
∠∠∠∠++++−−−−====
−−−−========
δ δδ δ
δ δδ δ
−−−−∠∠∠∠−−−−∠∠∠∠++++−−−−====
10 1
Z Z Z T
AC δ δδ δ
If EA=EB=1.0 pu
(((( ))))(((( ))))
−−−−
−−−−====
++++−−−−++++−−−−====
++++++++++++−−−−====
++++∠∠∠∠++++∠∠∠∠−−−−∠∠∠∠−−−−∠∠∠∠
++++∠∠∠∠++++∠∠∠∠++++−−−−====
2 cot
2 Z j Z
2 Z
sin 2
cos 1 j
2
1Z Z
sin j 2
sin j cos 1Z Z
10 110 1
10 1
Z Z
T A
T
T A
T A
T A
δ δδ δ
δ δδ δ
δ δδ δ
δ δδ δ
δ δδ δ δ δδ δ
δ δδ δ δ δδ δ
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During a swing, the angle δ changes.Fig. 13.37 shows the locus of Z C as a
function of δ on an R-X diagram, whenEA=EB
Fig. 13.37 Locus of Z C as a function of δδδδ, with E A=E B
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• When E A and E B are equal, the locus of Z C is seen to be a straight line which is theperpendicular bisector of the total system impedance between A and B, i.e., of theimpedance ZT
– the angle formed by lines from A and B to
any point on the locus is equal to thecorresponding angle δ
• When δ=0, the current I is zero and Z C is infinite
• When δ=180°, the voltage at the electrical centre is zero
– the relay at C in effect will see a 3-phasefault at the electrical centre. The electricalcentre and impedance centre coincide inthis case.
• If E A is not equal to E B , the apparent impedance loci are circles, with their centres onextensions of the impedance line AB
• When E A>E B , the electrical centre will be above the impedance centre; when E A<E B ,
the electrical centre will be below the impedance centre. Fig. 13.38 illustrates theshape of the apparent impedance loci for three different values of the ratio E A / E B .
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Fig. 13.38 Loci of ZC with different values of EA/EB
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• For generators connected to the main system through a weak transmission system (high external impedance), the electrical centre may appear on the transmission line
• When a generator is connected to the main system through a strong transmission system , the electrical centre will be in the step up transformer or possibly within the
generator itself• Electrical centres in effect are not fixed points: effective machine reactance and the
magnitudes of internal voltages vary during dynamic conditions.
• Voltage at the electrical centre drops to zero as δ increases to 180°and thenincreases in magnitude as δ increases further until it reaches 360°
– when δ reaches 180 , the generator willhave slipped a pole ; when δ reaches theinitial value where the swing started, one
slip cycle will have been completed.