بسم هللا الرحمن الرحيم رب اشرح لى صدرى ويسر لى أمر واحلل عقدة من لسانى يفقهوا قولى صدق هللا العظيم Chapter 11 Overhead Line Insulators part 2 pp. 370-389 Potential Distribution over a String of Suspension Insulators p. 376 • The voltage across the discs of the string is not uniformly distributed. This is because of the capacitances formed between the metal parts of the insulators and tower structure. • These capacitances could be made negligibly small by increasing the distance between the insulators and the tower structure which requires larger lengths bigger size of the towers and hence it becomes uneconomical. 4/17/2013 Prof. Dr. Magdi El-Saadawi 3 4/17/2013 Prof. Dr. Magdi El-Saadawi 4 4/17/2013 Prof. Dr. Magdi El-Saadawi 5 • In practice the insulators are not very far from the tower structure and hence these capacitances affect the voltage distribution across the string • Since the insulator discs are identical, each disc is represented by its mutual capacity C • A shunt capacitance C1 is the capacitance of metal part of the insulator disc to the tower structure (ground). So that C1 = m C • Where m is the ratio between the capacitance to ground to the mutual (unit) capacitance 4/17/2013 Prof. Dr. Magdi El-Saadawi 6 • Let V be the operating voltage and V1,V2,V3 and V4 the voltage drops across the units starting from cross towards the power conductor. V = V 1 + V2 + V3 + V4 • The objective is to find out the voltage across each disc as a multiple of the operating voltage and to compare the voltage across each unit. 4/17/2013 Prof. Dr. Magdi El-Saadawi 7 C : capacitance of each insulator unit. C1 = m C : capacitance to ground is the capacitance of metal part of the insulator unit to the tower (m<1). V1, V2, V3 the voltage across each unit starting from the cross arm towards the power conductor. V = V1 + V2 +V3 4/17/2013 Line voltage Prof. Dr. Magdi El-Saadawi 8 At point P: I2 = I1 +Ic1 ωC.V2 = ωC.V1 + ωmC.V1 V2 = (1+m).V1 At Point Q: I3 = I2 + Ic2 ωC.V3 = ωC.V2 + ωmC.(V1+V2) V3=m.V1 +(1+m).V2 =(m +(1+m)2).V1 V3 = (1+3m +m2).V1 4/17/2013 Prof. Dr. Magdi El-Saadawi 9 The voltage across the units cam also given by: n= 1 V2 = (1+ m). V1 n=2 V3 = (1+ 3 m +m2 ). V1 n=3 V4 = V3.(1+ 6 m +5 m2 + m3 ). V1 n=4 V5= V4.(1+ 10 m + 15 m2 + 7m3 + m4 ). V1 4/17/2013 Prof. Dr. Magdi El-Saadawi 10 To Find the voltage across each disk • For 3 disc string: • V = V1 + V2 + V3 • V = V1 + V1 (1+ m) + V3 (1+ 3m + m2) • V = V1 (3 + 4 m + m2) • Then you can find V1 , V2 and V3 • Where V: Voltage across the insulator string, (phase Volt) 4/17/2013 Prof. Dr. Magdi El-Saadawi 11 For m < 1 V 3 > V2 > V 1 Insulator (String) Efficiency: %η = (V/n.Vmax) x 100 V: Voltage across the insulator string, (phase Volt) n: number of insulator units. Vmax: Voltage across the insulator unit near to the power line (for n = 3, Vmax = V3). 4/17/2013 Prof. Dr. Magdi El-Saadawi 12 Example (1) Find the voltage distribution of an insulator of 3 units, if the maximum voltage of each unit is 17 kV, and the capacitance to ground is 20% of unit capacitance, also find the insulator efficiency. 4/17/2013 Prof. Dr. Magdi El-Saadawi 13 V3 = 17 kV, m=20% = 0.2 V2 = (1+m).V1 = 1.2 V1 V3 = (1+ 3 m +m2 ). V1 =1.64 V1 V1 = 17/1.64 = 10.36 kV V2 = 1.2x10.36 = 12.43 kV V= V1 + V2 + V3 = 39.8 kV Insulator efficiency = (39.8/3x17)x100=78.03% 4/17/2013 Prof. Dr. Magdi El-Saadawi 14 In general, voltage across the units can given by: Vn+1 = Vn.(1+m) + (V1+V2+……+ Vn-1).m n= 1 V2 = (1+m). V1 n=2 V3 = V2.(1+m) + V1.m n=3 V4 = V3.(1+m) + (V1 +V2).m n=4 V5= V4.(1+m) + (V1 + V2 +V3).m 4/17/2013 Prof. Dr. Magdi El-Saadawi 15 Example (2) An insulator string for 66 kV line has 4 units. The capacitance to ground is 10% of the capacitance of each insulator unit. Find the voltage across each insulator unit and string efficiency. 4/17/2013 Prof. Dr. Magdi El-Saadawi 16 V2 = (1+m). V1 = 1.1 V1 V3 = V2.(1+m) + V1.m = 1.31 V1 V4 = V3.(1+m) + (V1 +V2).m =1.651 V1 V1 +V2 +V3 +V4 = = 38.1 kV V1 (1+1.1 +1.31+1.651)=38.1 V1=7.53 kV, V2= 8.28 kV, V3=9.86 kV, V4= 12.43 kV String efficiency = (38.1/4x12.43)x100=76.6% 4/17/2013 Prof. Dr. Magdi El-Saadawi 17 Improvement of String Efficiency Methods of Equalizing Potential (p.386) 1- Reducing the ground capacitance relative to the capacitance of insulator unit (reduce m where m = c1/c ): This can be done by increasing the length of cross arm and hence taller supporting tower which uneconomical. 4/17/2013 Prof. Dr. Magdi El-Saadawi 18 Improvement of String Efficiency 2- Grading of insulator units: It can be seen that the unequal distribution of voltage is due to the leakage current from the insulator pin to the tower structure. The solution is to use insulator units with different capacitances. This requires that unit nearest the cross arm should have minimum capacitance (maximum Xc) and the capacitance should increase as we go towards the power line. 4/17/2013 Prof. Dr. Magdi El-Saadawi 19 This means that in order to carry out unit grading, units of different types are required. This requires large stocks of different units which is uneconomical and impractical. 4/17/2013 Prof. Dr. Magdi El-Saadawi 20 Improvement of String Efficiency 3- Static Shielding (Guard Ring): ( )حلقة الحماية This method uses a large metal ring surrounding the bottom insulator unit and connected to the line. This ring is called a grading or guard ring which gives a capacitance which will cancel the charging current of ground capacitance. 4/17/2013 Prof. Dr. Magdi El-Saadawi 21 Guard ring serves two purposes: - Equalizing the voltage drop across each insulator unit. - protects the insulator against flash over. 4/17/2013 Prof. Dr. Magdi El-Saadawi 22 pp. 389 4/17/2013 Prof. Dr. Magdi El-Saadawi 23 4/17/2013 Prof. Dr. Magdi El-Saadawi 24 4/17/2013 Prof. Dr. Magdi El-Saadawi 25 4/17/2013 Prof. Dr. Magdi El-Saadawi 26 4/17/2013 Prof. Dr. Magdi El-Saadawi 27 4/17/2013 Prof. Dr. Magdi El-Saadawi 28 Example (3) A 3-unit insulator string with guard ring. The capacitance to ground and to guard ring are 25 % and 10 % of the capacitance of each unit. Determine the voltage distribution and string efficiency. 4/17/2013 Prof. Dr. Magdi El-Saadawi 29 4/17/2013 Prof. Dr. Magdi El-Saadawi 30 At point A: I1 + Iy = Ix + i1 0.1ωC.(V2+V3) + ωC.V2 = ωC.V1 + 0.25 ωC.V1 1.25 V1 -1.1 V2 -0.1 V3 =0.0 At point B: I2 + Iz = Iy + i2 0.1ωC.V3 + ωC.V3 = ωC.V2 + 0.25ωC.(V1+V2) 0.25 V1 + 1.25 V2 -1.1V3 =0.0 4/17/2013 Prof. Dr. Magdi El-Saadawi 31 Also: V1 + V2 + V3 = V Solve, to get: V1= 0.295V, V2 = 0.2985V, V3 = 0.406V η = V/(3x0.406V)x100= 82.1 % Find the voltage distribution and insulator efficiency without a guard ring. 4/17/2013 Prof. Dr. Magdi El-Saadawi 32