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作 者:孙金鑫 倪小军 葛剑 韩松博 龚正 SUN Jin-xin;NI Xiao-jun;GE Jian;HAN Song-bo;GONG Zheng(Institute of Plasma Physics,Chinese Academy of Sciences,Hefei 230031;University of Science and Technology of China,Hefei 230027;Advanced Energy Research Center,Shenzhen University,Shenzhen 518060;Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education and Guangdong Province,College of Optoelectronic Engineering,Shenzhen University,Shenzhen 518060)
机构地区:[1]中国科学院等离子体物理研究所,合肥230031 [2]中国科学技术大学,合肥230027 [3]深圳大学新能源研究中心,深圳518060 [4]深圳大学光电工程学院,光电子器件与系统(教育部/广东省)重点实验室,深圳518060
出 处:《核聚变与等离子体物理》2022年第3期308-313,共6页Nuclear Fusion and Plasma Physics
基 金:国家重点研发计划(2017YFE0300503)。
摘 要:针对22.5°真空室扇形模型,建立CFETR真空室在等离子体大破裂工况下的有限元分析模型。通过仿真计算得到真空室在等离子体破裂工况下的涡流分布、电磁力分布,并将电磁载荷导入结构场,分析真空室不同PS段的应力、形变等结果。计算得到最大薄膜弯曲应力位于PS1段,约53.9MPa,远小于许用应力值。结果表明,真空室设计满足等离子体破裂工况下的结构强度要求。In this paper,based on the model of the 22.5°vacuum vessel,a finite element analysis model of the CFETR vacuum vessel under the condition of plasma major disruption is established.Through simulation calculation,the eddy current and electromagnetic force distribution of the vacuum vessel under major disruption working conditions are obtained,and the electromagnetic load is introduced into the structure field.The stress and deformation of the different PS sections of the vacuum vessel are analyzed.The calculated maximum film bending stress is in the first section,about 53.9MPa,which is far less than the allowable stress value.The results show that the design of the vacuum vessel meets the structural strength requirements under plasma major disruption conditions.
分 类 号:TL622[核科学技术—核技术及应用]
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