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Electrical Power Systems

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has the following properties<br />

R<br />

S|<br />

T|<br />

2 j240 j120°<br />

b = e = e = b<br />

*<br />

2 ej<br />

3<br />

– *<br />

b = b<br />

b = 1<br />

2<br />

1+ b+ b = 0<br />

U<br />

V|<br />

W|<br />

Symmetrical Components 227<br />

...(9.1)<br />

If the phase sequence is acb (negative sequence) then<br />

V a = V a, V b = b V a, V c = b 2 V a<br />

It is assumed that the subscript 1, 2, 0 refer to positive sequence, negative sequence and<br />

zero sequence respectively.<br />

If V a , V b and V c represent an unbalanced set of voltage phasors, the three balanced sets are<br />

written as:<br />

(V a1, V b1, V c1) positive sequence set<br />

(V a2, V b2, V c2) negative sequence set<br />

(V a0, V b0, V c0) zero sequence set<br />

A set of (balanced) positive sequence phasors is written as<br />

V a1, V b1 = b 2 V a1, V c1 = b 2 V a1 ...(9.2)<br />

A set of (balanced) negative sequence phasors is written as<br />

V a2, V b2 = bV a2, V c2 = b 2 V a2 ...(9.3)<br />

A set of zero sequence phasors is written as<br />

V a0 , V b0 = V a0 , V c0 = V a0 ...(9.4)<br />

The three phasors (Va , Vb , Vc ) can be expressed as the sum of positive, negative and zero<br />

sequence phasors defined above.<br />

Thus we can write,<br />

Va = Va1 + Va2 + Va0 ...(9.5)<br />

Vb = Vb1 + Vb2 + Vb0 ...(9.6)<br />

Vc = Vc1 + Vc2 + Vc0 ...(9.7)<br />

igure 9.1 shows symmetrical components of the unbalanced phasors.<br />

ig. 9.1: Symmetrical Components of Unbalanced Voltage Phasors.

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