Analysis of Electric Field and Current Density for Different Electrode Configuration of XLPE Insulation
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2018-05-06 https://doi.org/10.14419/ijet.v7i3.36.29092 -
current density, cross linked polyethylene (XLPE), electric field, electrodes configuration, Finite Element Method (FEMM) software -
Abstract
The most important aspect influencing the circumstance and characteristics of electrical discharges is the distribution of electric field in the gap of electrodes. The study of discharge performance requires details on the variation of maximum electric field around the electrode. In electrical power system, the insulation of high voltage power system usually subjected with high electric field. The high electric field causes the degradation performance of insulation and electrical breakdown start to occur. Generally, the standard sphere gaps widely used for protective device in electrical power equipment. This project is study about the electric field distribution and current density for different electrode configuration with XLPE barrier. Hence, the different electrode configuration influences the electric field distribution. This project mainly involves the simulation in order to evaluate the maximum electric field for different electrode configuration. Finite Element Method (FEM) software has been used in this project to perform the simulation. This project also discusses the breakdown characteristics of the XLPE. The accurate evaluation of electric field distribution and maximum electric field is an essential for the determination of discharge behavior of high voltage apparatus and components. The degree of uniformity is very low for pointed rod-plane when compared to other two electrode configurations. The non- uniform electric distribution creates electrical stress within the surface of dielectric barrier. As a conclusion, when the gap distance between the electrodes increase the electric field decrease.
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References
[1] Arora, R., & Mosch, W. (2011). High voltage and electrical insulation engineering (Vol. 69). John Wiley & Sons.
[2] Ibrahim, O. E. (1988). Expression of the electric field distribution in rod-plane gaps. IEEE Transactions on Electrical Insulation, 23(3), 493–494. https://doi.org/10.1109/14.2392
[3] Ichikawa, N. (2007). Study on detection of negative corona discharge generated in rod-plane air gap by using external electrode method. Plasma Science and Technology, 9(6), 686–689. https://doi.org/10.1088/1009-0630/9/6/10
[4] Kara, a, Kalenderli, Ö., & Mardikyan, K. (2006). Effect of Dielectric Barriers To the Electric Field of Rod-Plane Air Gap. COMSOL Conference 2006.
[5] Lee, W., & Lee, J. (2018). Numerical Study on Alternating Current Breakdown Mechanism Between Sphere – Sphere Electrodes in Transformer Oil-Based Magnetic Nanofluids, 18(9), 6629–6634. https://doi.org/10.1166/jnn.2018.15713
[6] Mavroidis, P. N., Mikropoulos, P. N., & Stassinopoulos, C. A. (2012). Impulse behavior of dielectric-covered rod-plane air gaps. IEEE Transactions on Dielectrics and Electrical Insulation, 19(2), 632–640. https://doi.org/10.1109/TDEI.2012.6180258
[7] Michealrakis (2015). Electric field distribution of sphere-plane gaps. KTH School of Electrical Engineering, 1-52.
[8] Waters, R. T., Rickard, T. E. S., & Stark, W. B. (1968). Electric Field and Current Density in the Impulse Corona Discharge in a Rod/Plane Gap. Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences, 304(1477), 187–210. https://doi.org/10.1098/rspa.1968.0081
[9] Chen, S., Zeng, R., Zhuang, C., Yu, Z., & He, J. (2013). Switching impulse breakdown characteristics of large sphere-plane air gaps compared with rod-plane air gap. IEEE Transactions on Dielectrics
[10] Maruyama, S., Ishii, N., Shimada, M., Kojima, S., Tanaka, H., Asano, M., Kawakami, S. (2004). Development of a 500-kV DC XLPE cable system. Furukawa Review, (25), 47–52.
[11] Ahmad, M. H., Bashir, N., Ahmad, H., Jamil, A. A. A., & Suleiman, A. A. (2014). An Overview of Electrical Tree Growth in Solid Insulating Material with Emphasis of Influencing Factors Mathematical Models and Tree Suppression. TELKOMNIKA Indonesian Journal of Electrical Engineering, 12(8). https://doi.org/10.11591/telkomnika.v12i8.5556
[12] Radu, I., Acedo, M., Filippini, J. C., Notingher, P., & Ftutos, F. (2000).The effect of water treeing on the electric field distribution of XLPE. The consequences for the dielectric strength. IEEE Transactions on Dielectrics and Electrical Insulation, 7(6), 860-868.
[13] Sasamoto, R., Nomiyama, R., Izawa, Y., & Nishijima, K. (2017, October). Laser charging effect on metallic particle inserted between positive DC sphere and plane in air gap. In Electrical Insulation and Dielectric Phenomenon (CEIDP), 2017 IEEE Conference on (pp. 62-65). IEEE.
[14] Tu, D. M., Liu, W. B., Zhuang, G. P., Liu, Z. Y., & Kao, K. C. (1989). Electric breakdown under quasi-uniform field conditions and effect of emission shields in polyethylene. IEEE Transactions on Electrical Insulation, 24(4), 581-590.
[15] McIntyre, C. C., & Grill, W. M. (2001). Finite element analysis of the current-density and electric field generated by metal microelectrodes. Annals of biomedical engineering, 29(3), 227-235.
[16] Kamarudin,MS, Radzi,NH, Ponniran,A, R Abd-Rahman (2016).Simulation of electric field properties for air breakdown using COMSOL multiphysics,Clean Energy and Technology Conference,1-5.
[17] Ieda, M., Nagao, M., & Hikita, M. (1994). High-field conduction and breakdown in insulating polymers. Present situation and future prospects. IEEE transactions on dielectrics and electrical insulation, 1(5), 934-945.
[18] Nikonov, V., Bartnikas, R., & Wertheimer, M. R. (2001). The influence of dielectric surface charge distribution upon the partial discharge behaviour in short air gaps. IEEE transactions on plasma science, 29(6), 866-874.
[19] Takahashi, T., Okamoto, T., Ohki, Y., & Shibata, K. (2005). Breakdown strength at the interface between epoxy resin and silicone rubber-a basic study or the development of all solid insulation. IEEE transactions on dielectrics and electrical insulation, 12(4), 719-724.
[20] Dissado, L. A., & Fothergill, J. C. (1992). Electrical degradation and breakdown in polymers (Vol. 9). IET.
[21] Uchida, K., Kobayashi, S. I., Kawashima, T., Tanaka, H., Sakuma, S., Hirotsu, K. I., & Inoue, H. (1996). Study on detection for the defects of XLPE cable lines. IEEE Transactions on Power Delivery, 11(2), 663-668.
[22] McKean, A. L. (1976). Breakdown mechanism studies in cross-linked polyethylene cable. IEEE Transactions on Power Apparatus and Systems, 95(1), 253-260.
[23] R Abd-Rahman, A Haddad, MS Kamarudin, MFM Yousof, NAM Jamail (2016). Dynamic modelling of polluted outdoor insulator under wet weather conditions, IEEE International Conference on Power and Energy (PECon), 610-614.
[24] Thakurdesai PA, Kole PL & Pareek RP (2004), Evaluation of the quality and contents of diabetes mellitus patient education on Internet. Patient Education and Counseling 53, 309–313.
[25] Rosli,H., Othman,N.A., Jamail, N.A.M., Ismail,M.N. (2017), Potential And Electric Field Characteristics Of Broken Porcelain Insulator , International Journal Of Electrical And Computer Engineering (IJECE) , 12, 3114.
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How to Cite
Sunthrasakaran, N., Akmal Mohd Jamail, N., Ezani Kamarudin, Q., & Gunabalan, S. (2018). Analysis of Electric Field and Current Density for Different Electrode Configuration of XLPE Insulation. International Journal of Engineering & Technology, 7(3.36), 127-133. https://doi.org/10.14419/ijet.v7i3.36.29092Received date: 2019-05-01
Accepted date: 2019-05-01
Published date: 2018-05-06