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High-Fidelity Approximations for Extinction Probability Calculations

机译:灭绝概率计算的高逼真逼近

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摘要

A quantity that is frequently of interest in stochastic neutronics calculations is the probability of extinction (POE), or its complement, the survival probability. Even within the simplest stochastic point kinetics formulations, the POE is typically extracted from numerical calculations or approximated. An example of the latter strategy involves the truncation of the fission multiplicity distribution at two, resulting in the "quadratic approximation. " While this methodology yields closed-form results for the POE, it is valid only for supercritical multiplication near unity. In this technical note, we attempt to obviate fission multiplicity truncation in the construction of transient and infinite time limit closed-form POE solutions. In the infinite time limit, we arrive at the necessity of solving a quintic algebraic equation; we provide a brief discussion of the mature formalism available for solving quintic equations and generate a variety of simple representations using hypergeometric series. We evaluate and discuss both the new and existing approximations in the context of an example ~(235)U system and compare their validity over a range of supercritical multiplication factors.
机译:随机中子学计算中经常需要关注的一个数量是灭绝概率(POE)或它的补余,即生存概率。即使在最简单的随机点动力学公式中,POE通常也可以从数值计算中提取或近似。后一种策略的一个示例涉及将裂变多重性分布在2点处截断,从而导致“二次近似。”虽然此方法可为POE生成封闭形式的结果,但仅对接近于1的超临界乘法有效。在本技术说明中,我们试图消除瞬态和无限时限封闭形式POE解决方案构造中的裂变多重性截断。在无限时限内,我们得出了求解五次代数方程的必要性。我们简要讨论了可用于求解五次方程的成熟形式主义,并使用超几何级数生成了多种简单表示形式。我们在示例〜(235)U系统的背景下评估和讨论了新的和现有的近似值,并比较了它们在一系列超临界倍增因子上的有效性。

著录项

  • 来源
    《Nuclear science and engineering》 |2013年第2期|197-205|共9页
  • 作者单位

    Los Alamos National Laboratory, X-Computational Physics Division MS F644, Los Alamos, New Mexico 87545;

    Los Alamos National Laboratory, X-Computational Physics Division MS F644, Los Alamos, New Mexico 87545;

  • 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 00:43:10

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