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Evaluation of the Induced to Spontaneous Fission Neutron Multiplicity Distribution Coefficients for Passive Neutron Multiplicity Counting of Plutonium and MOX

机译:Fi和MOX被动中子多重性计数的自发裂变中子多重性分布系数的评估

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Shift Register based passive neutron multiplicity counting of PuO2 or MOX samples relies on models to interpretthe measured data. To attain the highest accuracy these models require an appropriate description of the neutron multipletsproduced in the nuclear material. In order to account for the differences in neutron multiplicity distributions between theinitial spontaneous fission events and subsequent prompt induced fission events, a series of correction coefficients must bederived. These coefficients, the so-called κ?coefficients, are introduced into the neutron multiplication terms of the passiveneutron multiplicity counting interpretative model. They are expressed as overlap integrals involving the isotopiccomposition of the sample, the first three factorial moments of the induced (νI1, νI2, νI3) and spontaneous (νS1, νS2, νS3)fission neutron multiplicity distributions, the induced fission cross section of the fissile isotopes and the energy spectra ofneutrons that induce fission. In the absence of experimental evaluation of the induced fission factorial moments as afunction of incident neutron energy for plutonium isotopes other than 239Pu, the authors have used a limited data set (239Pu,235U and 238U) in conjunction with a normal probability distribution model of emitted multiplicity to derive approximatevalues of all of the important induced fission factorial moments. Several empirical relationships between νI1,νI2 and νI3 as afunction of energy have been used to produce alternative values of these parameters in order to evaluate the sensitivity ofthe results to the approach adopted. Propagation of the uncertainties has been performed throughout the calculations so thatthe resulting κ values derived in this work could be used with confidence for the purpose of quantitative neutronmultiplicity counting.Having established a calculational scheme, κ-coefficients for doubles and triples counting of isotope enrichedPuO2 samples have been compared with those of typical reactor grade PuO2 and MOX. The principal findings of this studywere: firstly that κ-coefficients exhibit only a small dependence on the isotopic composition of a given type of plutoniumproduct; secondly that, for best accuracy, the neutron energy spectral effect from (α,n) neutrons should be accounted for,especially when material with a significant (α,n) contribution are encountered; finally, that significantly different values ofthe κ-coefficients should be used when MOX or PuO2 material assay is performed.
机译:PuO2或MOX样品的基于移位寄存器的被动中子多重计数依靠模型来解释 测量数据。为了获得最高的精度,这些模型需要对中子多重峰进行适当的描述 在核材料中产生的。为了解决中子之间多重性分布的差异 最初的自发裂变事件和随后的瞬时诱发裂变事件,必须将一系列校正系数设为 衍生的。这些系数,即所谓的κ系数,被引入到无源的中子倍增项中。 中子多重计数解释模型。它们表示为涉及同位素的重叠积分 样品的成分,诱导的前三个阶乘矩(νI1,νI2,νI3)和自发的(νS1,νS2,νS3) 裂变中子的多重分布,裂变同位素的诱导裂变截面和能谱 诱发裂变的中子。在没有实验评估的诱导裂变阶跃矩的情况下, 239Pu以外的p同位素的入射中子能的函数,作者使用了有限的数据集(239Pu, 235U和238U)结合发射多重性的正态概率分布模型来得出近似值 所有重要的诱发裂变阶跃矩的数值。 νI1,νI2和νI3之间的几个经验关系为 能量的函数已被用来产生这些参数的替代值,以评估能量的敏感性。 所采用方法的结果。在整个计算过程中都进行了不确定性的传播,因此 在这项工作中得出的结果κ值可以放心地用于定量中子的目的 多重计数。 建立了计算方案后,同位素富集的两倍和三倍计数的κ系数 已将PuO2样品与典型反应堆级的PuO2和MOX样品进行了比较。这项研究的主要发现 分别是:首先,κ系数对给定类型of的同位素组成仅表现出很小的依赖性 产品;其次,为了获得最佳准确性,应考虑来自(α,n)中子的中子能谱效应, 特别是遇到具有重大(α,n)贡献的材料时;最后,那明显不同的价值 当进行MOX或PuO2材料测定时,应使用κ系数。

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