首页> 外文会议>The 13th International Conference on Nuclear Engineering: Abstracts >Study of the Melt-Cool down in a Suggested Core Catcher Concept for aHelium Cooled Fast Breeder Reactor after a Hypothetical Severe Accidentusing Computational Fluid Dynamics Simulation
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Study of the Melt-Cool down in a Suggested Core Catcher Concept for aHelium Cooled Fast Breeder Reactor after a Hypothetical Severe Accidentusing Computational Fluid Dynamics Simulation

机译:假设性严重事故后使用计算流体动力学模拟对建议的堆芯捕集器概念进行研究,该堆芯概念用于氦冷却的快中子增殖堆

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To ensure safety and containment during arnmeltdown of a fast breeder reactor core, arnhypothetical case has been considered andrnsimulated via computational fluid dynamics inrnwhich the entire core of a helium cooled fastrnbreeder reactor (875 MWth.) is melted down. Arn"core catcher concept" is suggested whichrnshould encapsulate the core melt. Its thermalrnperformance can only be determined through arnCFD-analysis. The device consists of a graph-iternhemisphere embedded in a two-layer blockrncomposed of concrete and zirconium dioxide,rnwhich serve as thermal insulators. The graph-iternis surrounded with a steel liner on whichrncooling channels are mounted to provide cool-ingrnat the outer shell throughout the meltdownrnprocess. Inside the graphite shell there is arnsolid steel bed. At the beginning of the melt-downrnsimulation, two liquid phases are as-sumedrnto be present in the core catcher: ura-niumrndioxide and contaminated molten steel. Inrnboth phases there is an internal heat sourcerndue to the radioactive decay of the fissionrnproducts present. This heat source power is arnfunction of the reactor thermal power, the timernthat the reactor has been operating underrnnormal conditions, and the time after shut-down.rnThe simulation was performed using thernvolume of fluid (VOF) and phase change mod-elsrnwithin the FLUENT CFD tool. It is foundrnthat once the core melt is in the core catcher,rnthe steel bed begins to melt, and the flow do-mainrnconsists of a colder flow falling downwardrnnear the side walls, an unstable zone in thernbulk with strong turbulence, and a stratifiedrnzone beneath it where heat transfer is domi-natedrnby conduction. The denser uranium diox-idernsinks and eventually solidifies. This is fol-lowedrnby re-melting of the uranium dioxide duernto reduced natural convection of liquid steel atrnthe base of the core catcher. After 26 hours, arnquasi-steady state is achieved in which bothrnphases remain at their respective melting tem-peratures, with a crust of considerable thick-nessrnforming covering the molten steel andrnuranium dioxide beneath it.
机译:为了确保快速增殖反应堆堆芯熔解过程中的安全性和密闭性,已考虑了无假想的情况,并通过计算流体动力学模拟了这种情况,氦冷却的快繁反应堆(875 MWth。)的整个堆芯都融化了。提出了应该包封芯熔体的“芯捕集器概念”。它的热性能只能通过arnCFD分析来确定。该设备由嵌入在由混凝土和二氧化锆组成的两层砖块中的图-半球组成,它们用作热绝缘体。由钢衬里包围的图样钢,在其上安装了冷却通道,以在整个熔化过程中在外壳上提供冷却。石墨壳内部有arnsolid钢床。在熔融模拟开始时,假定在捕集器中存在两种液相:铀-二氧化铀和受污染的钢水。在两个相中,由于存在的裂变产物的放射性衰变,存在内部热源。该热源功率是反应堆热功率的函数,反应堆在正常条件下运行的时间以及停机后的时间是函数。函数是在FLUENT CFD中使用流体体积(VOF)和相变模型进行模拟的工具。研究发现,一旦岩心融化在岩心捕集器中,钢床便开始熔化,流动主要是由较冷的流体向下下落到侧壁附近,大湍流中的不稳定区域和位于其下方的分层区域组成的。传热受传导支配的地方。较浓的铀二恶英吸附并最终固化。这是由于二氧化铀的重熔导致铁心捕集器底部钢水的自然对流减少而导致的。 26小时后,达到了安定稳态,其中两个相均保持在各自的熔化温度下,形成的厚皮形成了覆盖在其下方的钢水和二氧化铀。

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