02.07.2013 Views

Electrical Power Systems

Electrical Power Systems

Electrical Power Systems

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Eqns (6.15) and (6.17) can be written in matrix form.<br />

L<br />

V<br />

I SO<br />

NM SQP<br />

=<br />

L<br />

Characteristics and Performance of Transmission Lines 127<br />

O L<br />

I<br />

HG KJ QP<br />

NM<br />

ZYI<br />

1 +<br />

Z HG 2 KJ<br />

ZYI ZY<br />

Y 1 + 1 + HG 4 KJ 2<br />

NM<br />

Therefore, the ABCD constants for the nominal p model are given by<br />

<br />

HG I<br />

KJ<br />

+ HG I<br />

4 KJ<br />

ZY<br />

A = 1 + , B = Z,<br />

2<br />

C = Y 1<br />

6.5 LONG TRANSMISSION LINE<br />

V<br />

ZY ZY<br />

, D = 1 +<br />

2<br />

I<br />

R<br />

R<br />

O<br />

QP<br />

I<br />

HG KJ<br />

...(6.18)<br />

or short and medium length lines, accurate models were obtained by assuming the line<br />

parameters to be lumped. In case the lines are more than 250 km long, for accurate solutions<br />

the parameters must be taken as distributed uniformly along the length as a result of which the<br />

voltages and currents will vary from point to point on the line. In this section, expressions for<br />

voltage and current at any point on the line are derived. Then, based on these equations, an<br />

equivalent p model is obtained for long transmission line. igure 6.4 shows one phase of a<br />

distributed line of length l km.<br />

ig. 6.4: Schematic diagram of a long transmission line with<br />

distributed parameters.<br />

rom KVL, we can write,<br />

V(x + Dx) = z.Dx.I(x) + V(x)<br />

\ Vx x Vx<br />

( + D ) - ( )<br />

= z.I(x)<br />

Dx<br />

...(6.19)<br />

As Dx ® 0<br />

dV ( x)<br />

= z.I(x) ...(6.20)<br />

dx

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!