1 H、16 O、239 Pu和240 Pu截面不确定度产生Keff的敏感性和不确定度分析

A. Ahmed, H. Boukhal, T. E. Bardouni, O. Hajjaji, M. Makhloul, S. E. Ouahdani, M. Kaddour
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引用次数: 1

摘要

在核反应堆的临界和稳定性研究中,评估基本核数据(截面)的不确定性对不同中子参数的影响是非常重要的。因此,本工作对ENDF/B-VII中1H、16O、239Pu和240Pu同位素核数据的敏感性和不确定性进行了分析。1 .经最新版NJOY代码处理的横截面上的有效乘法系数。研究了不同IHECSBE基准的不同快速和热情况,计算了1H、16O、239Pu和240Pu同位素的灵敏度向量。利用蒙特卡罗代码MCNP6.1的Ksen卡,采用伴随加权摄动法计算了这些灵敏度向量。因此,将灵敏度向量与NJOY2016的ERRORJ模块生成的协方差矩阵相结合,计算核数据引起的不确定性。我们发现有几个截面和协方差矩阵缺乏调整:239Pu的俘获截面和裂变截面及其协方差矩阵缺乏热能调整。同一同位素的四种截面(弹性、非弹性、俘获和裂变)及其协方差矩阵均缺乏快速能量的调整。16 o;弹性截面及其协方差矩阵缺乏对热能的调整。1H的弹性截面和俘获截面及其协方差矩阵缺乏调整,特别是在热能方面。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Sensitivity and Uncertainty Analysis on the Keff Produced by the 1 H, 16 O, 239 Pu and 240 Pu Cross Sections Uncertainties
In criticality and stability studies of the nuclear reactor, it is important to evaluate the impact of the uncertainties of the basic nuclear data (cross sections) on the different neutron parameters. So this work is interested in the analysis of the sensitivity and uncertainties due to the nuclear data of 1H, 16O, 239Pu and 240Pu Isotopes in the ENDF/B-VII.1 cross sections processed by the latest version of NJOY code on the effective multiplication factor. Different rapid and thermal cases of the different IHECSBE benchmarks have been studied to calculate the sensitivity vectors for 1H, 16O, 239Pu and 240Pu Isotopes. These sensitivity vectors are calculated by using the adjoint-weighted perturbation method based on the Ksen card of the Monte Carlo code MCNP6.1. Thus, the uncertainties induced by nuclear data have been calculated by combining the sensitivity vectors with the covariance matrices that are generated by the ERRORJ module of NJOY2016. We found several cross sections and covariance matrices lack the adjustment: The capture and fission cross sections of the 239Pu and their covariance matrices lack the adjustment in the thermal energies. And all of the four cross sections (elastic, inelastic, capture and fission) and their covariance matrices for the same isotope lack the adjustment in the rapid energies. For 16O; the elastic cross section and its covariance matrix lack the adjustment in the thermal energies. The elastic and capture cross sections of the 1H and their covariance matrices lack the adjustment especially in the thermal energies.
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