铍中的瞬态中子谱和慢豫时间

P.S. Grover, L.S. Kothari
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引用次数: 2

摘要

用时间步长法对扩散近似中的玻尔兹曼方程进行了数值求解,以确定不同大小的铍组件内快中子爆发后的瞬态中子谱。该研究还给出了基模衰减常数和弛豫时间的信息。我们发现对于B2 <4 × 10−2 cm2时,长时间的衰变常数和中子能量分布与用迭代法计算的相应量吻合得很好。然而,对于较大的B2,直到所研究的时间(初始爆发后600 μsec)还没有建立平衡。与GAERTTNER等人的测量值进行了时间相关中子谱的比较,得到了无限组合体的慢豫时间为114 μsec。这一结果与ZHEZHERUN等人的测量结果进行了比较,他们报告的值要高得多:185±20 μsec。讨论了造成这种差异的可能原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Transient neutron spectra and the slowing down relaxation time in beryllium

The Boltzmann equation in the diffusion approximation has been numerically solved by the time-step method to determine transient neutron spectra, following a burst of fast neutrons inside beryllium assemblies of various sizes. Such a study also gives information about the decay constant of the fundamental mode and the slowing down relaxation time. We find that for B2 < 4 × 10−2 cm, the decay constant as well as the neutron energy distribution at long,times agrees well with the corresponding quantities calculated by an iteration procedure. However, for larger B2 up to the time investigated (600 μsec after the initial burst) equilibrium is not established. Timedependent neutron spectra have been compared with the measurements of GAERTTNER et al.

The slowing down relaxation time for an infinite assembly comes out to be 114 μsec. This result is compared with the measurements of ZHEZHERUN et al. who report a considerably higher value: 185 ± 20 μsec. The possible causes of this difference are discussed.

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