ASDEX 升级版和 JET 上的氦等离子体运行,以支持热核实验堆的非核阶段

A. Hakola, M. Balden, Matteo Baruzzo, R. Bisson, S. Brezinsek, T. Dittmar, D. Douai, Michael G Dunne, L. Garzotti, M. Groth, Rafael Henriques, Laszlo Horvath, I. Jepu, E. Joffrin, A. Kappatou, D. Keeling, K. Krieger, Benoit Labit, Morten Lennholm, J. Likonen, A. Loarte, Peter Lomas, C. G. Lowry, M. Maslov, D. Matveev, R. Pitts, U. Plank, M. Rasinski, D. Ryan, S. Saarelma, S. Silburn, E. Solano, W. Suttrop, Tuomas J J Tala, Emmanuelle Tsitrone, N. Vianello, T. Wauters, A. Widdowson, M. Wischmeier
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引用次数: 0

摘要

直到最近,热核实验堆还在考虑在其初始运行阶段使用非核氢(H)或氦(He)等离子体,以将核激活保持在较低水平。为此,EUROfusion 联合会托卡马克利用特别工作组于 2022 年在 ASDEX 升级(AUG)和 JET 托卡马克上开展了专门的 He 实验活动,重点是 ELMy H 模式运行和等离子体壁相互作用过程,以及与氢或氘等离子体的比较。在纯 He 和 He+H 混合等离子体中,都可以实现 H 模式运行,但与在 H 或 D 等离子体中相比,需要付出更多努力才能获得稳定的等离子体情况。即使在 He 中 LH 转变的功率阈值较低,进入 I 型 ELMy 状态似乎需要同样多甚至比在 H 中更多的加热功率。在 AUG 上研究了共振磁扰动对 ELM 的抑制,但只有在 He 含量低于 19% 的等离子体中才有可能发生;这种意外行为的原因仍不清楚,目前正在寻求各种理论方法,以正确理解 ELM 抑制背后的物理学原理。钨(W)等离子体面元件(PFC)的侵蚀率比氢等离子体中的侵蚀率大一个数量级,这可以归因于等离子体中 He2+ 离子的突出作用。在 AUG 上的 H 模式 He 等离子体中,首次明确证明了纳米级结构(W 绒毛)的形成。然而,尽管发生模糊的主要条件已经满足,但在 JET 上却没有获得模糊产生的直接证据。原因可能是 ELM 对 W 的侵蚀、模糊生长和退火之间的竞争以及共沉积物覆盖表面之间的微妙平衡。
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Helium plasma operations on ASDEX Upgrade and JET in support of the non-nuclear phases of ITER
For its initial operational phase, ITER has until recently considered using non-nuclear hydrogen (H) or helium (He) plasmas to keep nuclear activation at low levels. To this end, the Tokamak Exploitation Task Force of the EUROfusion Consortium carried out dedicated experimental campaigns in He on the ASDEX Upgrade (AUG) and JET tokamaks in 2022, with particular emphasis put on the ELMy H-mode operation and plasma-wall interaction processes as well as comparison to H or deuterium (D) plasmas. Both in pure He and mixed He+H plasmas, H-mode operation could be reached but more effort was needed to obtain a stable plasma scenario than in H or D. Even if the power threshold for the LH transition was lower in He, entering the type-I ELMy regime appeared to require equally much or even more heating power than in H. Suppression of ELMs by resonant magnetic perturbations was studied on AUG but was only possible in plasmas with a He content below 19%; the reason for this unexpected behaviour remains still unclear and various theoretical approaches are being pursued to properly understand the physics behind ELM suppression. The erosion rates of tungsten (W) plasma-facing components (PFCs) were an order of magnitude larger than what has been reported in hydrogenic plasmas, which can be attributed to the prominent role of He2+ ions in the plasma. For the first time, the formation of nanoscale structures (W fuzz) was unambiguously demonstrated in H-mode He plasmas on AUG. However, no direct evidence of fuzz creation on JET was obtained despite the main conditions for its occurrence being met. The reason could be a delicate balance between W erosion by ELMs, competition between the growth and annealing of the fuzz, and coverage of the surface with co-deposits.
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