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核聚变与等离子体物理 ›› 2017, Vol. 37 ›› Issue (3): 354-360.DOI: 10.16568/j.0254-6086.201703019

• 核聚变工程技术 • 上一篇    下一篇

CFETR磁体系统的中子学计算及活化分析

乔世吉,蒋 帅,陈 志*,徐 榭   

  1. (中国科学技术大学核科学技术学院,合肥 230027)
  • 收稿日期:2016-03-28 修回日期:2017-01-25 出版日期:2017-09-15 发布日期:2017-09-14
  • 作者简介:乔世吉(1989–),男,山西左云人,硕士,从事聚变堆辐射防护研究。
  • 基金资助:

    国家自然科学基金(11375182)

Neutronics calculation and activation analysis for CFETR magnet system

QIAO Shi-ji, JIANG Shuai, CHEN Zhi, XU Xie   

  1. (School of Nuclear Science and Technology, USTC, Hefei 230026)
  • Received:2016-03-28 Revised:2017-01-25 Online:2017-09-15 Published:2017-09-14

摘要:

用蒙特卡洛中子输运程序(MCNPX)对中国聚变工程实验CFETR超导磁体进行中子学输运计算,利用欧洲活化计算程序FISPACT对其进行活化计算分析,针对计算结果重点分析了磁体系统的中子学剂量分布以及活化情况。计算结果表明,中子能量通量最大处出现在聚变堆内侧线圈处,为3.97×1014 MeV•m–2,在该条件下超导线圈可以满足设计要求。停机后磁体组件的活度为3.33×1010Bq•kg–1,停机10年后下降2个数量级达到6.14×108Bq•kg–1。研究结果验证了所使用的CFETR 3维模型满足初步设计条件。

关键词: CFETR, 超导磁体, 中子剂量率, 活度

Abstract:

The Monte Carlo neutron transport code (MCNPX) is used to carry on the neutronics calculation for CFETR magnet system, and its activation analysis is performed by FISPACT, a European activation calculation code, besides. The calculated results show that the max neutron energy flux is 3.97×1014MeV•m–2, which meets the design requirements of the superconducting coil under this condition. The activity of magnet assembly is 3.33×1010Bq•kg–1 when reactor is shut down, and after 10-year shut down, the activity reaches 6.14×108Bq•kg–1, which decreases two order of magnitude. Conclusively, the CFETR 3D model meets the preliminary design requirements and can provide some data support for the construction of CFETR.

Key words: CFETR, Superconducting magnet, Neutron dose rate, Activity

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