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Electrical Power Systems

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

Resistance and Inductance of<br />

Transmission Lines<br />

2.1 INTRODUCTION<br />

2<br />

<strong>Power</strong> system engineering is that branch of <strong>Electrical</strong> Engineering which concerns itself with<br />

the technology of generation, transmission and distribution of electrical energy. The power<br />

system growing into a vast and complex system represents one of the most vital systems in<br />

every modern nation. The basic purpose of a transmission network is to transfer electric energy<br />

from generating units at various locations to the distribution system which ultimately supplies<br />

the load. Transmission line also interconnect neighbouring power utilities which allows not<br />

only economic dispatch of electrical power within regions during normal conditions, but also<br />

transfer of power between regions during emergencies.<br />

An overhead transmission line consists of a group of conductors running parallel to each<br />

other and carried on supports which provide insulation between the different conductors and<br />

between each conductor and earth. A transmission line has four parameters—resistance,<br />

inductance, capacitance and shunt conductance. The shunt conductance accounts for leakage<br />

currents flowing across insulators and ionized pathways in the air. The leakage currents are<br />

negligible as compared to the current flowing in the transmission lines. The series resistance<br />

causes a real power loss in the conductor. The resistance of the conductor is very important in<br />

transmission efficiency evaluation and economic studies. The power transmission capacity of<br />

the transmission line is mainly governed by the series inductance. The shunt capacitance<br />

causes a charging current to flow in the line and assumes importance for medium and long<br />

transmission lines. These parameters are uniformly distributed throughout but can be lumped<br />

for the purpose of analysis on approximate basis.<br />

2.2 LINE RESISTANCE<br />

The dc resistance of a solid round conductor is given by<br />

R dc = r×l<br />

A<br />

where r = resistivity of conductor<br />

l = length of conductor<br />

A = cross sectional area of conductor<br />

...(2.1)

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