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Electrical Power Systems

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under the action of T, H and wx.<br />

or equilibrium,<br />

T x = H and T y = wx<br />

Taking moments about P,<br />

I<br />

HG KJ<br />

H.y = wx x<br />

2<br />

\ y = wx<br />

2H<br />

2<br />

Analysis of Sag and Tension 383<br />

...(15.53)<br />

or short span with small sag, T max – T min can be considered as small. Therefore T max »<br />

T min = H. or T = T max = T min = H.<br />

Therefore, eqn. (15.53) can be written as:<br />

2<br />

y = wx<br />

2T<br />

when x = L<br />

, y = d<br />

2<br />

\ d = wL<br />

8T<br />

Since T = H,<br />

Also<br />

2<br />

2<br />

d = wL<br />

8H<br />

rom eqns. (15.13) and (15.56), we get<br />

l = L<br />

<br />

HG<br />

2<br />

8d<br />

1 +<br />

3L<br />

2<br />

I<br />

KJ<br />

...(15.54)<br />

...(15.55)<br />

...(15.56)<br />

...(15.57)<br />

Example 15.1: A transmission line conductor has been suspended freely from two towers and<br />

has taken the form of a catenary that has c = 487.68 m. The span between the two towers is<br />

152 m, and the weight of the conductor is 1160 kg/km. Calculate the following:<br />

(a) Length of the conductor (b) Sag<br />

(c) Maximum and minimum value of conductor tension using catenary method.<br />

(d) Approximate value of tension by using parabolic method.<br />

Solution:<br />

(a) rom eqn. (15.12),<br />

l = 2H<br />

w<br />

since c = H<br />

w<br />

I<br />

HG KJ<br />

wL<br />

sinh<br />

2H

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