Numerical Simulation of Thermal Characteristics of Anodes by Pure Metal and CuCr Alloy Material in Vacuum Arc

被引:23
作者
Huang, Xiaolong [1 ]
Wang, Lijun [1 ]
Jia, Shenli [1 ]
Qian, Zhonghao [1 ]
Deng, Jie [1 ]
Shi, Zongqian [1 ]
机构
[1] Xi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Peoples R China
基金
中国国家自然科学基金;
关键词
Alloys; anode; numerical simulation; pure metal; thermal characteristics; AXIAL MAGNETIC-FIELD; CURRENT INTERRUPTION; TEMPERATURE; SURFACE;
D O I
10.1109/TPS.2015.2443811
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Anode material seriously influences the characteristics of vacuum arc and further affects the performance of medium-voltage vacuum switches when the interruption current is high. There are many materials used for electrode manufacture, and different materials are selected for different switches. For a pure metal, its performance usually cannot satisfy the actual requirement. To improve switch's performance, an alloy is usually used as an electrode material. In this paper, thermal processes of six kinds of metal anodes (including pure metal and alloy anodes) are simulated and researched. The physical parameters of the pure metals all come from experiment results directly or are fitted by the experimental data. The physical parameters of the CuCr alloys are derived from Cu and Cr parameters. Two kinds of temperature calculation methods are used, which are called melting and solidification model and equivalent specific heat method, respectively. Simulation results show that W and Mo anodes have the higher temperature than Cu, Cr, CuCr25, and CuCr50 anodes. A pure Cr anode has the largest melting width and highest saturated vapor pressure and evaporation energy. A Cu anode has the biggest melting depth. A W anode has the smallest melting width and depth. Axial temperature gradient is related to the thermal conductivity, and the Cr anode has the largest axial temperature gradient. The thermal characteristics of CuCr25 and CuCr50 anodes are located between the pure Cu and Cr anodes. There are two melting points appearing in the results of CuCr alloys, and between the two melting points, the alloy anodes are in solid-liquid mixture state.
引用
收藏
页码:2283 / 2293
页数:11
相关论文
共 20 条
[1]  
[Anonymous], 1988, CRC HDB CHEM PHYS, DOI DOI 10.1002/JCTB.280500215.2007
[2]  
[Anonymous], P 21 ICEC ZUR SWITZ
[3]   MODEL OF THE ANODE REGION IN A UNIFORM MULTI-CATHODE-SPOT VACUUM-ARC [J].
BOXMAN, RL ;
GOLDSMITH, S .
JOURNAL OF APPLIED PHYSICS, 1983, 54 (02) :592-602
[4]  
Dieter E. G., 1979, METALS HDB PROPERTIE, V2
[5]  
Dullni E., 1989, ABB REV, V89, P11
[6]   Influence of Current Interruption on V-t Characteristics of Vacuum Interrupters [J].
Furukawa, Takaaki ;
Ueda, Masato ;
Kumada, Akiko ;
Hidaka, Kunihiko ;
Ikeda, Hisatoshi ;
Sato, Shuji ;
Nishimura, Seisuke ;
Shimizu, Hiroyuki ;
Shioiri, Tetsu ;
Homma, Mitsutaka .
IEEE TRANSACTIONS ON PLASMA SCIENCE, 2013, 41 (08) :1896-1903
[7]   MELTING OF COPPER BY AN INTENSE AND PULSED HEAT-SOURCE [J].
GELLERT, B ;
EGLI, W .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1988, 21 (12) :1721-1726
[8]  
Gmelin L., 1989, GMELIN HDB INORGANIC
[9]   THE HIGH-CURRENT METAL VAPOR ARC COLUMN BETWEEN SEPARATING ELECTRODES [J].
HEBERLEIN, JVR ;
GORMAN, JG .
IEEE TRANSACTIONS ON PLASMA SCIENCE, 1980, 8 (04) :283-288
[10]  
Klinski-Wetzel K. V., 2014, P 27 INT C EL CONT D, P1