期刊文献+

基于铜超比优化的管内电缆导体设计的数值模拟 被引量:1

Numeric simulation of CICC design based on optimization of ratio of copper to superconductor
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摘要 在铜超比优化的基础上,针对管内电缆导体结构设计,提出了数值模拟设计,进行了数值模拟设计,并将数值模拟设计结果与工程设计值进行了比较和分析,二者基本吻合。 For cable-in-conduit conductor (CICC) structure design, a numeric simulation is proposed for conductor configuration based on optimization of ratio of copper to superconductor. The simulation outcome is in agreeement with engineering design one.
出处 《核聚变与等离子体物理》 CAS CSCD 北大核心 2007年第3期237-241,共5页 Nuclear Fusion and Plasma Physics
基金 博士基金项目(2006BS007)
关键词 管内电缆导体 数值模拟设计 Cable-in-conduit conductor Numeric simulation design
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参考文献5

  • 1Lawrence Dresner. Twenty years of cablie-in-conduit conductors, 1975-1995 [J]. Joural of Fusion Enery, 1995, 14(1): 3.
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同被引文献9

  • 1李保增,郭增基.CICC超导体的设计及其稳定性[J].低温与超导,1995,23(2):17-22. 被引量:6
  • 2武松涛,吴维越,潘引年,陈文革,毕延芳,陈灼民,陈思跃,郁杰,吴杰峰,卫靖,武玉,翁佩德,高大明.EAST超导托卡马克装置中的大型超导磁体技术[J].低温物理学报,2005,27(A02):1113-1120. 被引量:4
  • 3Kuang Guangli. A 40T hybrid magnet under constructionin China[ J ] . IEEE Transactions on Applied Supercon-dut-tivity, 2010,20(3):680 -683.
  • 4Mitchell N. Analysis of the effect of Nb3Sn strand ben-ding on CICC superconductor performance[ J]. Cryogen-ics ,2002,42(5) : 311 -325.
  • 5Tan YunFei, et al. Prediction of quench in cable in -conduit conductors considering current - sharing effect ofcopper[ J] . Cryogenics,2006,46(7 - 8):615 -618.
  • 6Teng Yuping, et al. Controlling for outer - diameter ofsuperconducting cable for PF Cable - In - Conduit Con-ductor of ITER[ J]. Cryogenics,2012,52(12).
  • 7Zhai Yuhu. Electro - mechanical modeling of Nb3SnCICC performance degradation due to strand bending andinterfilament current transfer[ J]. Cryogenics,2009,50(3): 149-157.
  • 8Tan YunFei, et al. The design of cable - in - conduitconductors for the superconducting outsert coils of a 40Thybrid magnet [ J ]. Superconductor Science Technol.,2009, 22: 025010.
  • 9Bottura L, et al. Analysis of electrical coupling param-eters in superconducting cables [ J ]. Cryogenics,2003,43(3 -5) : 233 -239.

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