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Monte Carlo Fuel Temperature Coefficient Estimation by an Adjoint-Weighted Correlated Sampling Method

机译:伴随加权相关抽样方法的蒙特卡洛燃料温度系数估计

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摘要

It is very time-consuming to obtain a high-precision Monte Carlo (MC) estimate of the fuel temperature reactivity coefficient (FTC) through direct subtraction of two reactivity values from MC calculations at two different fuel temperatures. As an alternative to the direct subtraction MC estimate of the FTC, this paper presents a new method based on the adjoint-weighted correlated sampling technique. The new method translates the change in fuel temperature as the corresponding changes in both the microscopic cross sections and the transfer probabilities in scattering kernels described by the free gas model. The effectiveness of the new method is examined through continuous-energy MC neutronics calculations for pressurized water reactor pin cell and CANDU pressurized heavy water reactor lattice problems. The isotope-wise and reaction-type-wise contributions to the FTCs in the two problems are examined for two free gas models: the constant-cross-section and the resonance-cross-section models. It is demonstrated that the new MC method can predict the reactivity change due to fuel temperature variation as accurately as the conventional, more time-consuming direct subtraction MC method.
机译:通过直接减去两个不同燃料温度下MC的反应性值来获得燃料温度反应性系数(FTC)的高精度蒙特卡洛(MC)估计非常耗时。作为FTC直接减法MC估计的替代方法,本文提出了一种基于伴随加权相关采样技术的新方法。新方法将燃料温度的变化转换为微观截面和自由气体模型描述的散射核中转移概率的相应变化。通过连续能量MC中子学计算方法对压水反应堆针单元和CANDU压水堆反应堆晶格问题的有效性检验了该新方法的有效性。对于两个自由气体模型:等截面模型和共振截面模型,研究了在两个问题中对FTC的同位素和反应类型贡献。结果表明,新的MC方法可以像传统的,耗时的直接减法MC方法一样准确地预测由于燃料温度变化而引起的反应性变化。

著录项

  • 来源
    《Nuclear science and engineering》 |2014年第2期|184-192|共9页
  • 作者

    Hyung Jin Shim; Chang Hyo Kim;

  • 作者单位

    Seoul National University 1 Gwanak-ro, Gwanak-gu, Seoul 151-744, Korea;

    Seoul National University 1 Gwanak-ro, Gwanak-gu, Seoul 151-744, Korea;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 00:42:56

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