Abstract:In this paper, a finite-element method (FEM) simulation program is developed to analyze the ionized field of bipolar bundled conductors. In the simulation, the subconductors in the conductor bundle are considered individually while the influence among the subconductors is taken into account. The initial value setting of the positive and negative space charge density near the surface of the subconductor is explained in detail. After the validity of the method is testified, the corona ionized field of ±800kV HVDC line is analyzed. The corona current generated from the bundled conductors, the ground current density and the electric field distribution are calculated. The impacts of the number of bundles, the bundle spacing and the monopolar component on the corona current are investigated. It is found that, the corona current decreases with the increase in the number of bundles, and the corona current increases with the increase in the bundle spacing. If the monopolar component is not included, the corona current will be over-estimated. The simulation results show that the design of the ±800kV HVDC line can satisfy the ground current density and electric field limits of environment control standards.
[1] 张宇, 魏远航, 阮江军. 高压直流单极离子流场的有限元迭代计算[J]. 中国电机工程学报, 2006, 26(23): 158-162. [2] Adamiak K. Adaptive approach to finite element modeling of corona fields[J]. IEEE Transactions on Industry Application, 1994, 30(2): 387-393. [3] Luo Z, Demerdash N A. A finite-element ballooning model for 2D eddy current open boundary problems for aerospace applications[J]. IEEE Transactions on Magnetics, 1992, 28(5): 2241-2243. [4] Abdel-Salam M, Farghally M, Abdel-Sattar S. Finite element solution of monopolar corona equation [J]. IEEE Transactions on Electrical Insulation, 1983, 18(2): 110-119. [5] Al-Hamouz Z. Finite element solution of monopolar corona as influenced by ion lifetime[C]. Proc. of IEEE-IAS Annual Meeting on Industry Applications, 1996, 4: 1919-1924. [6] Sarma M P. Analysis of corona losses on dc transmission lines: I-unipolar lines [J]. IEEE Transactions on Power Apparatus and Systems, 1969, PAS-88(5): 718-731. [7] Takuma T, Ikeda T, Kawamoto T. Calculation of ion flow fields of HVDC transmission lines by the finite element method [J]. IEEE Transactions on Power Apparatus and Systems, 1981, PAS-100(12): 4802- 4810. [8] Yu M, Kuffel E. A new algorithm for evaluating the fields associated with HVDC power transmission lines in the presence of corona and strong wind [J]. IEEE Transactions on Magnetics, 1993, 29(2): 1985-1988. [9] Abdel-Salam M, Al-Hamouz Z. Analysis of the monopolar ionized field as influenced by ion diffusion[J]. IEEE Transactions on Industry Application, 1995, 31(3): 484-493. [10] Abdel-Salam M, Al-Hamouz Z. Novel finite-element analysis of space-charge modified fields[C]. IEE Proc. Science, Measurement and Technology, 1994, 141(5): 369-378. [11] Abdel-Salam M, Farghally M, Abdel-Sattar S. Monopolar corona on bundle conductors[J]. IEEE Transactions on Power Apparatus and Systems, 1982, PAS-101(10): 4079-4089. [12] Abdel-Salam M, Abdel-Sattar S. Calculation of corona V-I characteristics on monopolar bundles using the charge simulation method[J]. IEEE Transactions on Dielectric and Electrical Insulation, 1989, 24(4): 669-679. [13] Al-Hamouz Z M. Monopolar corona on bundle wires as influenced by wind[J]. IEEE Transactions on Industry Application, 1987, IA-23(6): 984-989. [14] Sunaga Y, Sawada Y. Method of calculating ionized field of HVDC transmission lines and analysis of space charge effects on RI[J]. IEEE Transactions on Power Apparatus and Systems, 1980, PAS-99(2): 605-615. [15] Al-Hamouz Z M. Combined finite element-charge simulation computation of monopolar corona on bundle wires[C]. IEEE 33th Annual meeting, Industry Applications Conf., 1998, 3: 1988-1993. [16] Al-Hamouz Z M. Finite-element solution of monopolar corona on bundle conductors[J]. IEEE Transactions on Industry Application, 1999, 35(2): 380-385. [17] Sarma M P. Analysis of corona losses on dc transmission lines: II-Bipolar lines[J]. IEEE Transactions on Power Apparatus and Systems, 1969, PAS-88(10): 1476-1491. [18] Qin B L, Sheng J N, Yan Z, et al. Accurate calculation of ion flow field under HVDC bipolar transmission lines[J]. IEEE Transactions on Power Delivery, 1988, 3(1): 368-376. [19] Abdel-Salam M, Al-Hamouz Z. A finite-element analysis of the bipolar ionized field[J]. IEEE Transactions on Industry Application, 1995, 31(3): 477-483. [20] Al-Hamouz Z M, Abdel-Salam M. Improved calculation of finite-element analysis of bipolar corona including ion diffusion[J]. IEEE Transactions on Industry Application, 1998, 34(2): 301-309. [21] Al-Hamouz Z M. Adaptive finite-element ballooning analysis of bipolar ionized fields[J]. IEEE Transactions on Industry Application, 1996, 32(6): 1266-1277. [22] Taknma T, Kawamoto T. A very stable calculation method for ion flow field of HVDC transmission lines[J]. IEEE Transactions on Power Delivery, 1987, 2(1): 189-198. [23] Lu T B, Feng H, Zhao Z B, et al. Analysis of the electric field and ion current density under ultra high-voltage direct-current transmission lines based on finite element method[J]. IEEE Transactions on Magnetics, 2007, 43(4): 1221-1224. [24] 李秋玮, 赵宇明, 惠建峰. 直流电晕笼中的合成场强和离子电流的计算[J]. 高电压技术, 2008, 34(2): 285-288. [25] 林秀丽, 徐新华, 汪大翚. 双极HVDC线路离子流电场计算及影响因素[J]. 高电压技术, 2007, 33(10): 54-58. [26] Al-Hamouz Z M, Abdel-Salam M. Inception voltage of corona in bipolar ionized fields effect on corona power loss[J]. IEEE Transactions on Industry Applications, 1998, 34(1): 57-65.