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CALCULATION OF HEATING VALUES FOR THE HIGH FLUX ISOTOPE REACTOR

机译:高通量同位素反应器的加热值的计算

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Calculating the amount of energy released by a fission reaction (fission Q value) and the heating rate distribution in a nuclear reactor is an important part of the safety analysis. However, these calculations can become very complex. One of the codes that can be used for this type of analyses is the Monte Carlo transport code MCNP5. Currently it is impossible to calculate the Q value and heating rate disposition for delayed beta and delayed gamma particles directly from MCNP5. The purpose of this paper is to outline a rigorous method for indirectly calculating the Q values and heating rates in the High Flux Isotope Reactor (HFIR), based on previous similar studies carried out for very high-temperature reactor configurations. This method has been applied in this study to calculate heating rates for the beginning of cycle (BOC) and end-of-cycle (EOC) states of HFIR. In addition, the BOC results obtained for HFIR are compared with corresponding results for the Advanced Test Reactor. The fission Q value for HFIR was calculated as 200.2 MeV for the BOC and 201.3 MeV for the EOC. It was also determined that 95.1% and 95.4% of the heat was deposited within the HFIR fuel plates for the BOC and EOC models, respectively. This methodology can also be used for heating rate calculations for HFIR experiments.
机译:计算裂变反应释放的能量(裂变Q值)和核反应堆中的加热速率分布是安全分析的重要部分。但是,这些计算可能会变得非常复杂。可以用于这种类型的分析的代码之一是蒙特卡洛运输代码MCNP5。目前,无法直接从MCNP5计算延迟的β和延迟的γ粒子的Q值和升温速率。本文的目的是基于以前对极高温反应堆配置进行的类似研究,概述一种严格的方法,用于间接计算高通量同位素反应堆(HFIR)中的Q值和加热速率。该方法已用于本研究中,以计算HFIR的循环开始(BOC)和循环结束(EOC)状态的加热速率。此外,将HFIR获得的BOC结果与Advanced Test Reactor的相应结果进行比较。 HFIR的裂变Q值对于BOC计算为200.2 MeV,对于EOC计算为201.3 MeV。对于BOC和EOC模型,还确定分别有95.1%和95.4%的热量沉积在HFIR燃料板内。该方法还可以用于HFIR实验的加热速率计算。

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