EE356: Power Transmission, Distribution and Utilization Farhan Mahmood, PhD Department of Electrical Engineering UET, Lahore May 23, 2016 Outline • Capacitance of transmission lines • Transmission line parameters • Potential at a charged single conductor • Capacitance of single-phase transmission line • Capacitance of three-phase transmission line • Method of images Page 2 Field Lines Produced by Transmission Lines Page 3 Capacitance of Transmission Lines • The two parallel wires act as plates of a capacitor and that the air between them acts as a dielectric. • Capacitance also exists between the transmission line wires, as illustrated in figure. • The capacitance between the wires is usually expressed in picofarads per unit length. • This electric field between the wires is similar to the field that exists between the two plates of a capacitor. Page 4 Capacitance of Transmission Lines • Advantages of shunt capacitance of transmission lines: ˗ Reduction in line losses due to decrease in the magnitude of current ˗ Improved efficiency of transmission lines ˗ Reduction in voltage drop, and hence voltage regulation Page 5 Transmission Line Parameters • Since any dielectric, even air, is not a perfect insulator, a small current known as leakage current flows between the two wires. • In effect, the insulator acts as a resistor, permitting current to pass between the two wires. • Figure shows this leakage path as capacitors-resistors in parallel connected between the two lines. This property is called conductance (G) and is the opposite of resistance. Page 6 Potential at a Charged Single Conductor • We first compute the electric field of a uniformly charged, solid cylindrical conductor and the voltage between two points outside the conductor. • We also compute the voltage between two conductors in an array of charged conductors. • Gauss’s law states that the total electric flux leaving a closed surface equals the total charge within the volume enclosed by the surface, that is, the normal component of electric flux density integrated over a closed surface equals the charge enclosed: • where D ┴ denotes the normal component of electric flux density, E ┴ denotes the normal component of electric field strength, and ds denotes the differential surface area. Page 7 Potential at a Charged Single Conductor • From Gauss’s law, where ε = ε0 is the permittivity of free space • Electric field intensity at any point is the gradient of voltage, Page 8 Capacitance of Single-Phase Transmission Line • The Inductance of a single-phase lines can be expressed as below, Page 9 Capacitance of 3-Phase Transmission Line Symmetrical Spacing • Inductance per phase of three-phase line with symmetrical spacing (equilateral spaced soild conductor) is given by, Page 10 Exercise Problem 1: • A 3-phase, 132 kV, 50 Hz, transmission line has an equilateral spacing of 1.5 m, diameter of each conductor is 1.5 cm. Calculate the capacitive reactance of the line if the length of the line is 100 km. Also, calculate the charging current in amp per km length of the line. Page 11 Capacitance of 3-phase Transmission Line • The average capacitance per phase is given by, Page 12 Capacitance of 3-Phase, Double Circuit Line Double Circuit Transmission Line r’ Page 13 Capacitance of 3-Phase, Double Circuit Line Page 14 Capacitance of 3-Phase, Bundled Conductor Line Page 15 Conductor Tables Inductive reactance at 1 feet spacing (Xa) Inductive reactance spacing factor (Xd) Page 17 Method of Images (or Mirror Charges) Page 18 Method of Images (or Mirror Charges) Page 19 Capacitance of 1-phase Transmission Line Considering the Effect of Ground Page 20 Exercise Problem 2: • A single-phase transmission line consists of two conductors spaced at a distance of 1.2 m, the diameter of each conductor is 1.5 cm. Assuming that the height of the line from the ground is 8 m, calculate capacitance between conductors and capacitance from conductor to ground for the following cases: (a) ignoring the effect of ground (b) considering the effect of ground. Page 21 CLO-1 • Apply the concept of flux linkages and voltage drop in the calculation of inductance and capacitance of transmission lines. Page 22 THANK YOU FOR YOUR ATTENTION