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Electrical Power Systems

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

The elastic property of wire is measured by its modulus of elasticity. The modulus of<br />

elasticity is defined as the stress per unit area divided by the deformation per unit length.<br />

Since<br />

s = T<br />

A kg/m2<br />

where<br />

s = stress per unit area (kg/m2 )<br />

T = conductor tension (kg)<br />

A = actual cross section of conductor (m 2 )<br />

Elongation e of the conductor due to the tension is<br />

e =<br />

stress<br />

modulus of elasticity<br />

... (15.1)<br />

... (15.2)<br />

Elongation is high if modulus of elasticiy is low. Thus, a small change in the length of<br />

conductor causes large effect on sag and tension of conductor.<br />

Sag and stresses in conductors are dependent on the following things:<br />

1. Initial tension put on them when they are clamped in place.<br />

2. Weight of the conductors themselves.<br />

3. Ice or sleet chinging to them.<br />

4. Wind pressure.<br />

Stress depends on sag, any span can be used provided the poles or towers are high enough<br />

and strong enough. The matter is merely one of extending the catenary in both directions. Cost<br />

of towers sharply increases with height and loading.<br />

15.2 EECT O TEMPERATURE CHANGE<br />

Sag and stress vary with temperature because of the thermal expansion and contraction of the<br />

conductor. Temperature rise of conductor increase the length of conductor, and hence sag<br />

increases and tension decreases. A temperature fall causes opposite effect. Maximum stress<br />

occurs at the lowest temperature, when the line has contracted and is also possibly covered with<br />

ice and sleet.<br />

If conductor stress is constant while the temperature changes, the change in length of the<br />

conductor is<br />

Dl = l 0 aDt ...(15.3)<br />

where<br />

Dt = t 1 – t 0, Dl = l 1 – l 0<br />

where<br />

t 0 = initial temperature<br />

l 0 = conductor length at initial temperature t 0<br />

l 1 = conductor length at t 1.<br />

a = coefficient of linear expansion of conductor per degree centigrade.<br />

Dt = change in temperature in degree centigrade.<br />

Dl = change in conductor length in meter.<br />

If the temperature is constant while the conductor stress changes (i.e., loading), the change<br />

in length of the conductor is

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