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首页> 外文期刊>Annals of nuclear energy >Calculation of the spallation target neutronic parameters in Accelerator Driven Subcritical TRIGA reactor
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Calculation of the spallation target neutronic parameters in Accelerator Driven Subcritical TRIGA reactor

机译:加速器驱动亚临界TRIGA反应堆中散裂目标中子参数的计算

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摘要

In this paper, effect of the spallation target neutronic parameters such as beam profile, proton beam energy (E-p), target thicknesses and for different materials in an Accelerator Driven Subcritical TRIGA reactor has been investigated. Monte Carlo code MCNPX has been used to calculate neutronic parameters such as: spallation neutron yield (Y-n/p), neutron spectrum, angular distribution of the spallation neutrons coming out of the target and spallation neutron production spectra in the target region for two cases of uniform and parabolic beam spatial distributions. According to the results, the relative difference of spallation neutron yield increases by 3.45% using a parabolic spatial distribution instead of a uniform spatial distribution and also this parameter increases by 7.91% using a thick target instead of a thin target, respectively. Moreover, with increasing E-p from 115 MeV up to 2 GeV, the relative difference of spallation neutron yield improves by 4813.58%. Additionally, in comparison to uniform spatial distribution of the proton beam, having parabolic spatial distribution has the advantage of more homogeneity in the spatial distribution of generated spallation neutrons as well as heat generation in the target. Also, Y-n/p/E-p parameter increases with target atomic number and proton beam energy. Therefore, our results are indicative of the fact that investigating sensitivity of the target spallation neutronic parameters is necessary in order to optimally design a cost-efficient Accelerator Driven Subcritical Reactors (ADSRs). (C) 2015 Elsevier Ltd. All rights reserved.
机译:在本文中,研究了加速器驱动的亚临界TRIGA反应堆中散裂目标中子学参数的影响,例如束轮廓,质子束能量(E-p),目标厚度以及不同材料的影响。蒙特卡罗代码MCNPX已用于计算中子参数,例如:两种情况下的散裂中子产率(Yn / p),中子谱,散落到目标的散裂中子的角度分布以及散裂中子在目标区域中的产生谱。均匀和抛物线形的空间分布。根据结果​​,使用抛物线空间分布而不是均匀空间分布,散裂中子产量的相对差增加了3.45%,并且使用厚靶而不是薄靶,该参数分别增加了7.91%。此外,随着E-p从115 MeV增加到2 GeV,散裂中子产率的相对差异提高了4813.58%。此外,与质子束的均匀空间分布相比,具有抛物线形空间分布的优点是,在生成的散裂中子的空间分布以及目标中的热量生成方面具有更高的同质性。而且,Y-n / p / E-p参数随着目标原子序数和质子束能量的增加而增加。因此,我们的结果表明以下事实:必须研究目标散裂中子学参数的灵敏度,才能优化设计经济高效的加速器驱动亚临界反应堆(ADSR)。 (C)2015 Elsevier Ltd.保留所有权利。

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