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Physics basis for the first ITER tungsten divertor

机译:第一个ITER钨分流器的物理基础

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On the eve of component procurement, this paper discusses the present physics basis for the first ITER tungsten (W) divertor, beginning with a reminder of the key elements defining the overall design, and outlining relevant aspects of the Research Plan accompanying the new “staged approach” to ITER nuclear operations which fixes the overall divertor lifetime constraint. The principal focus is on the main design driver, steady state power fluxes in the DT phases, obtained from simulations using the 2-D SOLPS-4.3 and SOLPS-ITER plasma boundary codes, assuming the use of the low Z seeding impurities nitrogen (N) and neon (Ne). A new perspective on the simulation database is adopted, concentrating purely on the divertor physics aspects rather than on the core-edge integration, which has been studied extensively in the course of the divertor design evolution and is published elsewhere. Emphasis is placed on factors which may increase the peak steady state loads: divertor target shaping for component misalignment protection, the influence of fluid drifts, and the consequences of narrow scrape-off layer heat flux channels. All tend to push the divertor into an operating space at higher sub-divertor neutral pressure in order to remain at power flux densities acceptable for the target material. However, a revised criterion for the maximum tolerable loads based on avoidance of W recrystallization, sets an upper limit potentially ~50% higher than the previously accepted value of ~10?MW?m?2, a consequence both of the choice of material and the finalized component design. Although the simulation database is currently restricted to the 2-D toroidally symmetric situation, considerable progress is now also being made using the EMC3-Eirene 3-D code suite for the assessment of power loading in the presence of magnetic perturbations for ELM control. Some new results for low input power corresponding to the early H-mode operation phases are reported, showing that even if realistic plasma screening is taken into account, significant asymmetric divertor heat fluxes may arise far from the unperturbed strike point. The issue of tolerable limits for transient heat pulses is an open and key question. A new scaling for ELM power deposition has shown that whilst there may be more latitude for operation at higher current without ELM control, the ultimate limit is likely to be set more by material fatigue under large numbers of sub-threshold melting events.
机译:在部件采购的前夕,本文讨论了第一个ITER钨(W)偏滤器的当前物理基础,首先提醒了定义总体设计的关键要素,并概述了伴随新“阶段性研究”而制定的研究计划的相关方面。 ITER核行动的“方法”,解决了总的滤清器寿命限制。主要重点在于主要设计驱动力,DT阶段的稳态功率通量,假设使用低Z籽晶杂质氮(N),则使用2-D SOLPS-4.3和SOLPS-ITER等离子边界代码通过仿真获得)和霓虹灯(Ne)。采用了关于仿真数据库的新视角,纯粹是在偏滤器的物理方面而不是在核心-边缘集成上进行了研究,该问题已在偏滤器设计的发展过程中进行了广泛研究,并在其他地方发表。重点放在可能增加峰值稳态负载的因素上:用于保护组件不对准的偏滤器目标形状,流体漂移的影响以及窄刮除层热通量通道的后果。为了保持在目标材料可接受的功率通量密度,所有趋向于将偏滤器以较高的子偏滤器中性压力推入工作空间。但是,基于避免W再结晶的最大容许载荷的修订标准,将上限设定为比先前公认的〜10?MW?m?2的值高约50%,这是材料和材料选择的结果。最终的组件设计。尽管仿真数据库目前仅限于2-D环形对称情况,但是使用EMC3-Eirene 3-D代码套件进行ELM控制的电磁扰动评估功率负载时,也正在取得可观的进步。据报道,与早期H模式运行阶段相对应的低输入功率的一些新结果表明,即使考虑到实际的等离子体屏蔽,远离不扰动的冲击点也可能会产生明显的不对称偏滤器热通量。瞬态热脉冲的容许极限问题是一个悬而未决的关键问题。一种新的ELM功率沉积定标表明,尽管在没有ELM控制的情况下,在更高电流下可能会有更大的工作自由度,但最终极限很可能由在大量次阈值熔化事件下的材料疲劳来设定。

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