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泡沫不锈钢层TRISO颗粒的堆内行为模拟

尹春雨 刘仕超 焦拥军 周毅 高士鑫 邢硕 青涛 汪丽达 闫新龙

尹春雨, 刘仕超, 焦拥军, 周毅, 高士鑫, 邢硕, 青涛, 汪丽达, 闫新龙. 泡沫不锈钢层TRISO颗粒的堆内行为模拟[J]. 核动力工程, 2021, 42(4): 133-137. doi: 10.13832/j.jnpe.2021.04.0133
引用本文: 尹春雨, 刘仕超, 焦拥军, 周毅, 高士鑫, 邢硕, 青涛, 汪丽达, 闫新龙. 泡沫不锈钢层TRISO颗粒的堆内行为模拟[J]. 核动力工程, 2021, 42(4): 133-137. doi: 10.13832/j.jnpe.2021.04.0133
Yin Chunyu, Liu Shichao, Jiao Yongjun, Zhou Yi, Gao Shixin, Xing Shuo, Qing Tao, Wang Lida, Yan Xinlong. In-Pile Performance of TRISO Particle Used Stainless Steel Foams as Buffer Layer[J]. Nuclear Power Engineering, 2021, 42(4): 133-137. doi: 10.13832/j.jnpe.2021.04.0133
Citation: Yin Chunyu, Liu Shichao, Jiao Yongjun, Zhou Yi, Gao Shixin, Xing Shuo, Qing Tao, Wang Lida, Yan Xinlong. In-Pile Performance of TRISO Particle Used Stainless Steel Foams as Buffer Layer[J]. Nuclear Power Engineering, 2021, 42(4): 133-137. doi: 10.13832/j.jnpe.2021.04.0133

泡沫不锈钢层TRISO颗粒的堆内行为模拟

doi: 10.13832/j.jnpe.2021.04.0133
基金项目: 国家自然科学基金项目(12005213)
详细信息
    作者简介:

    尹春雨(1982—),男,高级工程师,主要从事燃料元件及其相关组件设计和研究工作,E-mail: yincy909@163.com

  • 中图分类号: TL334

In-Pile Performance of TRISO Particle Used Stainless Steel Foams as Buffer Layer

  • 摘要: 三向同性燃料(TRISO)颗粒中疏松热解碳层堆内辐照收缩产生间隙后,会导致TRISO颗粒热导恶化。为解决该问题,本文采用泡沫不锈钢替代TRISO颗粒中的疏松热解碳层。对泡沫不锈钢TRISO颗粒的堆内行为模拟结果表明,采用泡沫不锈钢可以避免疏松层堆内密实化,提高疏松层的传热效率,有效降低核芯运行温度;不论采用泡沫不锈钢还是疏松热解碳作为疏松层,内层致密热解碳层(IPyC层)和外层致密热解碳层(OPyC层)的应力均会超过包覆层强度;碳化硅(SiC)层的环向应力随泡沫不锈钢层弹性模量的减小而减小,通过降低泡沫不锈钢弹性模量可以有效控制SiC层应力,保证其结构完整性。因此,应选取气孔率高、弹性模量低的泡沫不锈钢作为TRISO颗粒的疏松层,可在改善热导恶化问题的同时保证SiC层的结构完整性。该研究为TRISO颗粒在工程应用中的优化设计提供了指导。

     

  • 图  1  TRISO颗粒的计算模型

    Figure  1.  Computational Model of TRISO Particles

    图  2  寿期初TRISO颗粒径向温度分布状态

    Figure  2.  Radial Temperature Distribution of TRISO Particles at the Beginning of Life Period

    图  3  疏松热解碳-IPyC层、泡沫不锈钢-IPyC层尺寸变化

    Figure  3.  Size Changes between IPyC and Metal Foam-IPyC Layer    

    图  4  SiC层的应力状态随中子注量的变化曲线

    Figure  4.  Curves of Stress State of SiC Layer with Neutron Fluence     

    图  5  不同中子注量下IPyC层应力状态

    Figure  5.  Stress State of IPyC under Different Neutron Fluence

    图  6  不同中子注量下OPyC层应力状态

    Figure  6.  Stress State of OPyC under Different Neutron Fluence   

  • [1] MILLER G. Statistical approach and benchmarking for modeling of multi-dimensional behavior in TRISO-coated fuel particles[J]. Journal of Nuclear Materials, 2003, 317(01): 69-78. doi: 10.1016/S0022-3115(2)01702-6
    [2] SEN R S, POPE M A, OUGOUAG A M. Assessment of possible cycle lengths for fully encapsulated microstructure fueled light water reactor concepts[J]. Nuclear Engineering and Design, 2013, 255(1): 310-320.
    [3] SCHAPPEL D, TERRANI K, POWERS J, et al. Thermo mechanical analysis of fully ceramic microencapsulated fuel during in-pile operation[C]. United States: Top Fuel 2016, 2016.
    [4] HALES J D, WILLIAMSON R L. Multidimensional multiphysics simulation of TRISO particle fuel[J]. Journal of Nuclear Materials, 2013, 443(1): 531-543.
    [5] 辛勇,李垣明,唐昌兵,等. 金属基弥散微封装燃料中TRISO燃料颗粒的尺寸优化设计[J]. 核动力工程,2019, 40(2): 176-179.
    [6] LIU R Z, LIU M L, CHANG J X, et al. An improved design of TRISO particle with porous SiC inner layer by fluidized bed-chemical vapor deposition[J]. Journal of Nuclear Materials, 2015, 467(1): 917-926.
    [7] BESMANN T M, FERBER M K, LIN H T, et al. Fission product release and survivability of UN-kernel LWR TRISO fuel[J]. Journal of Nuclear Materials, 2014, 448(1): 412-419.
    [8] NOOR F M, ROSIP N M, JAMALUDIN K R, et al. Effect of sintering temperature on the properties of stainless steel foam[J]. Advanced Materials Research, 2015, 1807(1): 232-235.
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出版历程
  • 收稿日期:  2020-11-13
  • 修回日期:  2020-12-09
  • 刊出日期:  2021-08-15

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