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Measurement method of relative burnup distribution of irradiated fuel

机译:辐照燃料相对燃耗分布的测量方法

摘要

PURPOSE:To enable quick measurement in a shorter time than in the case of employment of a Ge semiconductor detector by determining the distribution of relative burnup of a fuel by the use of a large number of gamma-ray detectors disposed on the lateral sides of the fuel and by measuring the distribution therefrom. CONSTITUTION:When it is assumed that measurement of gross gamma-ray are executed at a plurality of points, a gross gamma-ray signal at an n-th measuring point is set as GGn, burnup at that point as BUn, a gross gamma-ray signal at a reference point as GGo and burnup at this point as BUo. From these values, the distributions gn=GGn/GGo and rn=BUn/BUo at the n-th measuring point are obtained. On the occasion, the burnup BUo is assumed to be known. By using an approximation formula, the distribution rn=gn.K (BUo, Tc)/K (Buo.gn, Tc) is led out. Tc is assumed to be a cooling period of a fuel. A factor expressed by a fraction in the right member of this formula represents a correction coefficient. The burnup distribution (rn) can be determined by substituting the distribution (gn), the burnup BUo and the cooling period Tc for a prescribed relation formula.
机译:目的:与使用锗半导体探测器的情况相比,通过使用布置在炉膛侧面的大量伽马射线探测器确定燃料的相对燃耗分布,可以在更短的时间内进行快速测量。燃料并测量其分布。组成:假设在多个点执行总伽马射线测量,则将第n个测量点的总伽马射线信号设置为GGn,在该点处的燃尽为BUn,总伽马射线在参考点处的射线信号为GGo,在该点处的燃尽为BUo。根据这些值,获得在第n个测量点处的分布gn = GGn / GGo和rn = BUn / BUo。在这种情况下,假定燃耗BUo是已知的。通过使用近似公式,导出分布rn = gn.K(BUo,Tc)/ K(Buo.gn,Tc)。假定Tc为燃料的冷却时间。在该公式的右半部分中用分数表示的因子表示校正系数。燃耗分布(rn)可以通过将分布(gn),燃耗BUo和冷却时间Tc代入规定的关系式而求出。

著录项

  • 公开/公告号JP2845471B2

    专利类型

  • 公开/公告日1999-01-13

    原文格式PDF

  • 申请/专利权人 TOSHIBA KK;

    申请/专利号JP19890016363

  • 发明设计人 KUMANOMIDO HIRONORI;

    申请日1989-01-27

  • 分类号G21C17/06;

  • 国家 JP

  • 入库时间 2022-08-22 02:29:44

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