首页> 外文会议>Mathematics and Computations, Supercomputing in Nuclear Applications and Monte Carlo International Conference >ANALYSIS OF TEMPERATURE EFFECTS ON REACTIVITY OF LIGHT WATER REACTOR FUEL ASSEMBLIES BY USING MVP-2 ADOPTING AN EXACT RESONACE ELASTIC SCATTERING MODEL
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ANALYSIS OF TEMPERATURE EFFECTS ON REACTIVITY OF LIGHT WATER REACTOR FUEL ASSEMBLIES BY USING MVP-2 ADOPTING AN EXACT RESONACE ELASTIC SCATTERING MODEL

机译:MVP-2采用精确的共振弹性散射模型对轻水反应堆燃料反应性的温度影响分析

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The Japan Atomic Energy Agency has installed a resonance elastic scattering model coupled with the thermal motion of target nucleuses (the exact model) to the continuous energy Monte Carlo code MVP-2 and also prepared the libraries of elastic scattering cross sections at 0 K for ~(235)U, ~(238)U, ~(238)Pu, ~(239)Pu, ~(240)Pu, ~(241)Pu, ~(242)Pu and ~(241)Am, which are necessary to apply the exact model. We applied the code and the libraries to analyze the neutron multiplication factors (k_(inf)'s) and Doppler reactivity of UO_2 and MOX fuel assemblies for light water reactors, and compared them with those obtained by using the conventional asymptotic slowing down model (the asymptotic model). The base condition of the assemblies was a hot operating condition with an in-channel void fraction of 40% and a fuel pellet temperature of 520 °C (793 K) for the BWR fuel assemblies and a hot zero power condition with that of 284 °C (557 K) for the PWR fuel assemblies. From the base condition only fuel pellet temperatures was raised to 1500 °C (1773 K). The calculated results showed that the difference in k_(inf)'s between the exact and the asymptotic models were -220 to -410 pcm (1 pcm=0.00001 Δk) at the 1500°C condition, and the exact model made the Doppler reactivity between the base and the 1500°C conditions more negative by 7 to 10%. The effect of the exact model for all the heavy isotopes other than ~(238)U was to make the Doppler reactivity less negative by a few %.
机译:日本原子能机构已经安装了与靶核(精确模型)的热运动耦合到连续能量蒙特卡罗代码MVP-2的谐振弹性散射模型,并在0 k下制备了弹性散射横截面的文库。 (235)U,〜(238)U,〜(238)PU,〜(239)PU,〜(240)PU,〜(241)PU,〜(242)PU和〜(241)AM,这是必要的应用确切的模型。我们应用了代码和图书馆来分析中子倍增因子(K_(INF)的燃料组件的中子倍增因子(K_(INF)的燃料组件,并将其与通过使用常规渐近减速模型获得的那些(渐近模型)。组件的碱条件是热操作条件,其具有40%的通道空隙率和520°C(793 k)的燃料颗粒温度,用于BWR燃料组件和具有284°的热零功率条件C(557 K)用于PWR燃料组件。从基础条件下,只有燃料颗粒温度升至1500℃(1773 k)。计算结果表明,在1500°C条件下,精确和渐近模型之间的K_(INF)的差异为-220至-410pcm(1 pcm = 0.00001Δk),精确模型使多普勒反应性在碱和1500℃之间的条件下,更负数为7%至10%。除〜(238)u以外的所有沉重同位素的确切模型的影响是使多普勒反应性小于阴性的少量%。

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