Boron Equivalent Measurement of Nuclear Graphite with Photoneutron Source

被引:0
|
作者
Wang X. [1 ,2 ,3 ]
Hu J. [1 ,2 ]
Chen J. [1 ,2 ,3 ]
Cai X. [1 ,2 ,3 ]
Wang N. [1 ,2 ,3 ]
Wang H. [4 ]
Han J. [1 ,2 ]
机构
[1] Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai
[2] CAS Innovative Academies in TMSR Energy System, Shanghai
[3] University of Chinese Academy of Sciences, Beijing
[4] Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai
关键词
Boron equivalent; MCNP simulation; Nuclear graphite; Photoneutron source;
D O I
10.7538/yzk.2019.youxian.0781
中图分类号
学科分类号
摘要
Impurities in nuclear materials with high thermal neutron absorption cross section will change the reactivity. The absorption of thermal neutrons by these impurities is represented by boron equivalent, which is one of the important factors to measure the purity of nuclear materials. Boron equivalent can be determined directly via the measurement of macroscopic thermal neutron absorption cross section based on an isotopic neutron source, but with lower accuracy. The photoneutron source, which can generate neutrons with higher intensity, better direction and lower energy, can effectively improve the accuracy of boron equivalence measurement. Therefore, the boron equivalent measurement of nuclear graphite was carried out with the photoneutron source driven by 15 MeV electron LINAC. Monte Carlo simulation method was used to optimize the experimental scheme, and the experimental data were tested and modified. Finally, the quantitative analysis method was established for the measurement of graphite boron equivalent. This method can quickly and accurately measure the boron equivalent of nuclear materials, which is of great significance for the physical design and safety assessment of the reactor. © 2020, Editorial Board of Atomic Energy Science and Technology. All right reserved.
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页码:1991 / 1998
页数:7
相关论文
共 20 条
  • [1] ZHAO Mu, Study on related problems of nuclear graphite for high temperature gas-cooled reactor, Nuclear Safety, 13, 4, pp. 34-38, (2014)
  • [2] JIANG Mianheng, XU Hongjie, DAI Zhimin, Advanced fission energy program-TMSR nuclear energy system, Bulletin of the Chinese Academy of Sciences, 27, 3, pp. 366-374, (2012)
  • [3] VIRGIL'EV YU S., Impurities in and service ability of reactor graphite, Atomic Energy, 84, 1, pp. 6-13, (1998)
  • [4] ZHAO Jing, LI Fu, WEI Chunlin, Boron depletion in high-temperature gas-cooled reactor, Atomic Energy Science and Technology, 46, 2, pp. 172-175, (2012)
  • [5] Guidelines for nuclear transfers, INFCIRC/254/Rev.5/Part 1, (2002)
  • [6] ROBERTSON R C., MSRE design and operations report, Part I: Description of reactor design, ORNL-TM-728, (1965)
  • [7] CHEN Zhong, ZHAO Zijia, LV Zhongliang, Et al., Coaxial stacking disjoint model study of 10 MW high temperature gas-cooled reactor (HTR-10), Nuclear Engineering and Design, 353, (2019)
  • [8] HE Nanling, LI Xiujuan, JIANG Guodu, Et al., Determination of impurity element in neptunium dioxide power by ICP-AES, Atomic Energy Science and Technology, 53, 3, pp. 539-545, (2019)
  • [9] YIN Liangliang, TIAN Qing, SHAO Xian-zhang, Et al., ICP-MS measurement of uranium and thorium contents in minerals in China, Nuclear Science and Techniques, 27, 1, pp. 61-64, (2016)
  • [10] LI Jinying, WANG Fan, ZHAO Yonggang, Et al., Recent research and process of laser mass spectrometry, Atomic Energy Science and Technology, 46, 10, pp. 1165-1174, (2012)