Puissance residuelle totale emise par les produits de fission thermique DE 235U

M. Lott, G. Lhiaubet, F. Dufreche, R. de Tourreil
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引用次数: 9

Abstract

In this paper we present some new results concerning the β + γ residual power following the 235U thermal fission for cooling times going from 70 to 7 × 104 s.

We give a brief description of the experimental technique and of the methods used to obtain the residual power from the measurements. Then we examine the different sources of errors. The residual power curves for three different irradiation times as well as a curve due to one fission (elementary fission curve) are given.

These experimental results are compared with other values coming from β and γ measurements and from theoretical calculations based on fission products systematics. For the considered cooling times the discrepancies between our experimental results and the theoretical calculations are less than 12% for cooling times <700 s and inside the experimental uncertainties for cooling times > 700 s.

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235U热裂变产物释放的总剩余功率
本文给出了235U热裂变后冷却时间从70到7 × 104 s的β + γ剩余功率的一些新结果。我们简要地描述了实验技术和从测量中获得剩余功率的方法。然后我们检查不同的误差来源。给出了三种不同辐照时间的剩余功率曲线和一次裂变的剩余功率曲线(初等裂变曲线)。这些实验结果与来自β和γ测量和基于裂变产物系统学的理论计算的其他值进行了比较。对于考虑的冷却时间,我们的实验结果与理论计算之间的差异小于12%,冷却时间为700秒,在冷却时间的实验不确定度之内。700年代。
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The neutron yield from Li, Be, Co and Cu under proton bombardment at energies from 5 to 10 MeV The emission spectra of NaD2O, InBe, LaBe and NaBe photoneutron sources Neptunium-237 production and recovery An exact solution of a transcendental equation basic to the theory of intermediate resonance absorption of neutrons Mathematical theory of transport processes in gasesJ. H. Ferziger and H. G. Kaper, North Holland, Amsterdam (1972). pp. 579
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