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Study of global wall saturation mechanisms in long-pulse ELMy H-mode discharges on JT-60U

机译:JT-60U上长脉冲ELMy H型放电的整体壁饱和机理研究

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Variation of particle absorption at the first wall has been investigated in long-pulse (~ 30 s) ELMy H-mode discharges on JT-60U. Quantitative analysis of particle balance indicated that particle inventory at the first wall was globally saturated with a time scale of 10-15 s after several long-pulse discharges. To understand mechanisms of the global wall saturation, distribution of a local wall saturation time on the first wall was calculated from the ion and neutral particle fluxes to the first wall evaluated using a Monte-Carlo neutral particle transport code. The local wall saturation time was estimated to be shorter than 1 s at the divertor plates and the divertor dome, ~ 10 s at the lower half of the baffle plates and ~ 100s at the main chamber wall, respectively. This result suggested that the divertor plates, the divertor dome and the lower half of the baffle plates were saturated in a single discharge. On the other hand, the main chamber wall was not saturated in a single discharge. Based on the above result, a model of the global wall saturation was proposed, where dynamic and static inventory regions are defined depending on the wall temperature.
机译:在JT-60U上的长脉冲(〜30 s)ELMy H模式放电中,已经研究了第一壁颗粒吸收的变化。颗粒平衡的定量分析表明,在多次长脉冲放电后,第一壁的颗粒存量总体上处于饱和状态,时间尺度为10-15 s。为了了解整体壁饱和的机理,使用蒙特卡洛中性粒子传输代码,根据到第一壁的离子和中性粒子通量,计算了第一壁上局部壁饱和时间的分布。在分流板和分流器圆顶处,局部壁的饱和时间估计短于1 s,在挡板的下半部分别为〜10 s,在主室壁处为〜100 s。该结果表明,分流板,分流器穹顶和挡板的下半部分在一次放电中就饱和了。另一方面,主腔室壁在一次放电中并未饱和。基于以上结果,提出了整体墙体饱和度的模型,其中根据墙体温度定义了动态和静态库存区域。

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