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Second-Order Sensitivity Analysis of Uncollided Particle Contributions to Radiation Detector Responses

机译:非碰撞粒子对辐射探测器响应的二阶灵敏度分析

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This work presents an application of Cacuci’s Second-Order Adjoint Sensitivity Analysis Methodology (2nd-ASAM) to the simplified Boltzmann equation that models the transport of uncollided particles through a medium to compute efficiently and exactly all of the first- and second-order derivatives (sensitivities) of a detector’s response with respect to the system’s isotopic number densities, microscopic cross sections, source emission rates, and detector response function. The off-the-shelf PARTISN multigroup discrete ordinates code is employed to solve the equations underlying the 2nd-ASAM. The accuracy of the results produced using PARTISN is verified by using the results of three test configurations: (1) a homogeneous sphere, for which the response is the exactly known total uncollided leakage, (2) a multiregion two-dimensional (r-z) cylinder, and (3) a two-region sphere for which the response is a reaction rate. For the homogeneous sphere, results for the total leakage as well as for the respective first- and second-order sensitivities are in excellent agreement with the exact benchmark values. For the nonanalytic problems, the results obtained by applying the 2nd-ASAM to compute sensitivities are in excellent agreement with central-difference estimates. The efficiency of the 2nd-ASAM is underscored by the fact that, for the cylinder, only 12 adjoint PARTISN computations were required by the 2nd-ASAM to compute all of the benchmark’s 18 first-order sensitivities and 224 second-order sensitivities, in contrast to the 877 PARTISN calculations needed to compute the respective sensitivities using central finite differences, and this number does not include the additional calculations that were required to find appropriate values of the perturbations to use for the central differences.
机译:这项工作提出了Cacuci的二阶伴随敏感性分析方法(2nd-ASAM)在简化的Boltzmann方程中的应用,该方程对未碰撞粒子通过介质的传输进行建模,从而可以有效,准确地计算所有一阶和二阶导数(灵敏度)相对于系统的同位素数密度,微观横截面,源发射率和探测器响应函数的探测器响应。使用现成的PARTISN多组离散纵坐标代码来求解2nd-ASAM的方程式。通过使用三种测试配置的结果来验证使用PARTISN产生的结果的准确性:(1)均质球体,其响应是确切已知的总非碰撞泄漏;(2)多区域二维(rz)圆柱体(3)一个两区域的球体,其响应为反应速率。对于均质球体,总泄漏量以及相应的一阶和二阶灵敏度的结果与确切的基准值非常吻合。对于非解析问题,通过应用2nd-ASAM计算灵敏度获得的结果与中心差估计值非常一致。相比之下,第二个ASAM的效率得到了强调,对于圆柱体,第二个ASAM仅需要进行12个伴随的PARTISN计算即可计算基准的18个一阶灵敏度和224个二阶灵敏度。使用中心有限差分来计算相应灵敏度所需的877 PARTISN计算的结果,该数字不包括找到用于中心差分的扰动的适当值所需的其他计算。

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