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Ion orbit modelling of ELM heat loads on ITER divertor vertical targets

机译:ITER分流器垂直靶上ELM热负荷的离子轨道建模

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Highlights ? ELM heat loads to tungsten monoblocks in ITER are calculated. ? Larmor radius effects focus power onto toroidal edges. ? There is no margin against edge melting in the pre-nuclear phase at half current, half field. ? Edge melting will occur in the nuclear phase of ITER operation. Abstract The high heat flux areas on the vertical divertor targets in the ITER tokamak will consist of cuboid tungsten monoblocks bonded to copper cooling tubes. Three-dimensional ion orbit modelling is used to calculate the heating of tungsten monoblocks during ELMs at the inner vertical target, where the highest surface energy densities are expected. The presence of thin gaps between monoblocks results in exposed edges onto which the heat flux can be focused. ELM ions are focused by their gyromotion onto the magnetically shadowed, long toroidal edges of the monoblocks. The risk of monoblock edge melting is greater than the risk of full surface melting on the plasma-wetted zone. Alternative shaping solutions such as edge chamfering, filleting, and poloidal beveling do not show promise; the melt zone simply migrates to other locations on the monoblocks. Without ELM mitigation, there is a marginal risk of edge melting due to uncontrolled ELMs in the pre-nuclear phase of ITER operation, and an absolute certainty of it in the burning nuclear phase. To avoid edge melting altogether, the surface energy density would have to limited to less than 0.15MJ/m 2 .
机译:强调 ?计算了ITER中钨单体的ELM热负荷。 ?拉莫尔半径效应将功率聚焦到环形边缘上。 ?在半电流半场的情况下,在核前相中没有防止边缘熔化的余量。 ?边缘熔化将发生在ITER操作的核阶段。摘要ITER托卡马克垂直分流器靶上的高热通量区域将由长方体钨单块粘结到铜冷却管上。三维离子轨道建模用于计算内部垂直目标在ELM期间钨单块的加热,在内部垂直目标中,预期表面能量密度最高。单体之间存在细小的间隙会导致暴露的边缘,热流可以聚焦在该边缘上。 ELM离子的旋转运动将其聚焦在整体式磁屏蔽的长环形边缘上。整体边缘熔化的风险大于等离子润湿区域上整个表面熔化的风险。诸如倒角,倒角和倒角倒角之类的其他成形解决方案并未显示出希望;熔体区只是迁移到单体上的其他位置。如果没有缓解ELM,由于在ITER操作的核前阶段不受控制的ELM,边缘熔化的边际风险很小,而在燃烧核阶段则有绝对的确定性。为了避免边缘完全融化,表面能密度必须限制为小于0.15MJ / m 2。

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