3ππ Year Electric Power REPORT Transmission Lines β« Ψ£ΨΩ Ψ― Ω ΨΩ Ψ― ΨΨ³Ω ΨΉΨ§ΩΩ β¬/ β«Ψ§Ψ§ΩΨ³Ω β¬ Sec./ 2 B.N/ 29 1|Page List of contents • Introduction • Transmission Line Parameters I. Resistance II. Inductance III. capacitance • Performance of Transmission Lines • Conclusion • References List of figures I. II. Skin effect Two Parallel Wires with Single–Phase Circuit III. Single-Phase Line double circuit IV. Unbalanced Three–Phase Line V. VI. VII. VIII. IX. Single Phase Two-wire Line conductors and a neutral point between them Phase Overhead Line with equal spacing Phase Overhead Line with unequal spacing Single Phase Short Transmission Lines X. Medium Transmission Lines Nominal π Method XI. Medium Transmission Lines Nominal T Method XII. Long Transmission Lines 2|Page Introduction Transmission lines is a very important part of electrical system as it is used to carry large amount of generated power at very high voltage from one station to another. we are going to study the transmission line parameters and its performance. 1. Transmission Line Parameters Transmission lines have the electrical properties resistance, inductance and capacitance. 1. Series resistance: due to resistivity of conductors material. 2. Series inductance: due to magnetic field produced by ac current. 3. Shunt capacitance: due to electric field from potential difference between conductors. 1.1. Resistance of overhead transmission line DC resistance is calculated by Where: ρ is conductor resistivity at a given temperature (β¦.m) L is conductor length (m) A is cross-section area (m2) If AC current is flowing, rather than DC current, the conductor effective resistance is higher due to skin effect. Skin Effect • The alternating current concentrating near the surface of a conductor (see figure 1) is known as skin effect. • The effective area of cross-section of the conductor is reduced. • The resistance of the conductor is increased when carrying an ac current. 3|Page Figure 1 Skin effect Temperature Effect As temperature rises, the conductor resistance increases linearly, over normal operating temperatures, according to the following equation: 1.2. Inductance of overhead transmission line When an alternating current flows in lines, a changing magnetic flux is produced. The changing flux links the lines, and the lines possesses inductance. It depends on • Size of conductor (r). • Distance between conductors (D). • Material of conductors (π) 1. Inductance of Two Parallel Wires with Single–Phase Circuit π·π πΏ = 2 ∗ 10−7 πΏπ( ) π·π Dm= D DS=re-0.25 Figure 2 Two Parallel Wires with Single–Phase Circuit 4|Page 2. Inductance of Single-Phase Line double circuit πΏ = 2 ∗ 10−7 πΏπ( Where: π·π = 2∗2√π· π·π π·π ) ππ₯ π·ππ¦ π· ππ₯ π·ππ¦ 2 π·π = 2 √ππ π·ππ ππ π·ππ Figure 3 Single-Phase Line double circuit 3. Inductance of a Three–Phase Line a) Balanced Three–Phase Line π· πΏ = 2 ∗ 10−7 πΏπ( ) π·π DS=re-0.25 Figure 4 Balanced Three–Phase Line b) Unbalanced Three–Phase Line π·π πΏ = 2 ∗ 10−7 πΏπ( ) π·π π·π = 3√π·π΄π΅ π·π΅πΆ π·πΆπ΄ DS=re-0.25 Figure 5 Unbalanced Three–Phase Line 1.3. Capacitance of Overhead transmission lines If we have two conductors separated from each other by an insulator and have a potential difference, there will be capacitance between them. In transmission lines conductors there is potential difference between any two conductors and they are separated by air so they will exhibit capacitance effect. 5|Page We need to calculate the capacitance to consider it while design of transmission lines. A. Capacitance of a Single Phase Two-wire Line 1. capacitance between two wires A is equal to B d Figure 6 Single Phase Two-wire Line 2. capacitance between one of the conductors and a neutral point between them is equal to A N B Figure 7 conductors and a neutral point between them B. Capacitance of a 3-Phase Overhead Line 1. Equal spacing Capacitance between conductor and neutral is equal to equal to πΆπβ = 2ππ0 π· π ln( ) 2. Unequal spacing Capacitance between conductor and neutral is equal to πΆπβ = Figure 8 3-Phase Overhead Line with equal spacing 2ππ0 π· ln( π ) π·π where π·π = 3√π·π΄π΅ π·π΅πΆ π·πΆπ΄ π·π = π 6|Page Figure 9 3-Phase Overhead Line with unequal spacing 2. Performance of Transmission Lines To study the Performance of Transmission Lines we will study some terms such voltage drop, line losses and efficiency of transmission which will indicate how successfully is the design and operation of a transmission line. So first we will represent the transmission line and study it mathematically. Classification of Overhead Transmission Lines 1. Short transmission lines: • The length of an overhead transmission line is up to about 80 km. • The capacitance effects are small and is neglected. Figure 10 Single Phase Short Transmission Lines 2. Medium transmission lines: • The length of an overhead transmission line is between 80 km and 240 km. • The capacitance effects are considered. Figure 12 Medium Transmission Lines Nominal π Method 7|Page Figure 11Medium Transmission Lines Nominal T Method 3. Long transmission lines: • The length of an overhead transmission line is more than 240 km. • The line constants are considered uniformly distributed over the whole length of the line. Figure 13 Long Transmission Lines ,For mathematical analysis we will use Two Port Network Where: • Vr, Ir are the receiving end voltage, current. • Vs, Is are the sending end voltage, current. • To calculate values of A, B, C and D for all cases: Table 1 Long A cosh π B Zsinh π π 8|Page Medium π Medium T Short 1 Z Z C Ysinh π π D cosh π • • • • • Y 0 (Because y=0 and Is=Ir ) 1 R: Total resistance of the line X: Inductive reactance of the line Z: Total line impedance B: Capacitive susceptance 1 Y: Admittance Y= = π½π΅ ππΆ • π = √ππ Now we will define voltage regulation, line losses and efficiency of transmission. 1. voltage regulation The difference in voltage at the receiving end of a transmission line and the sending end and is expressed as a percentage of the receiving end voltage. 2. Line losses ππΏππππΈπ = πππΈππ·πΌππΊ − ππ πΈπΆπΈπΌππΌππΊ 3. Transmission efficiency The ratio of receiving end power to the sending end power of a transmission line 9|Page Conclusion As transmission lines is a very important part of electrical system we have illustrated 1. The transmission line parameters (their meanings and how to calculate them): • Resistance • Inductance • Capacitance 2. The transmission line performance by viewing short, medium and long representation of it and defining voltage regulation, line losses and efficiency of transmission. References I. II. III. Principles of Power Systems By V.K Mehta 4th edition . Power System Analysis - Hadi Saadat. Lectures notes. 10 | P a g e