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Studies of the pedestal structure and inter-ELM pedestal evolution in JET with the ITER-like wall

机译:ITER样壁的JET的基座结构和ELM基座之间的演化研究

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摘要

The pedestal structure of type I ELMy H-modes has been analysed for JET with the ITER-like Wall (JET-ILW). The electron pressure pedestal width is independent of ρ ~∗ and increases proportionally to √β _(pol,PED). Additional broadening of the width is observed, at constant β _(pol, PED), with increasing ν ~∗ and/or neutral gas injection and the contribution of atomic physics effects in setting the pedestal width cannot as yet be ruled out. Neutral penetration alone does not determine the shape of the edge density profile in JET-ILW. The ratio of electron density to electron temperature scale lengths in the edge transport barrier region, η _e, is of order 2-3 within experimental uncertainties. Existing understanding, represented in the stationary linear peeling-ballooning mode stability and the EPED pedestal structure models, is extended to the dynamic evolution between ELM crashes in JET-ILW, in order to test the assumptions underlying these two models. The inter-ELM temporal evolution of the pedestal structure in JET-ILW is not unique, but depends on discharge conditions, such as heating power and gas injection levels. The strong reduction in p _(e,PED) with increasing D _2 gas injection at high power is primarily due to clamping of ∇ T _e half way through the ELM cycle and is suggestive of turbulence limiting the T _e pedestal growth. The inter-ELM pedestal pressure evolution in JET-ILW is consistent with the EPED model assumptions at low gas rates and only at low beta at high gas rates. At higher beta and high gas rate the inter-ELM pedestal pressure evolution is qualitatively consistent with the kinetic ballooning mode (KBM) constraint but the peeling-ballooning (P-B) constraint is not satisfied and the ELM trigger mechanism remains as yet unexplained.
机译:对于具有类ITER墙(JET-ILW)的JET,已经对类型I ELMy H-mode的基座结构进行了分析。电子压力的基座宽度与ρ〜∗无关,并且与√β_(pol,PED)成比例地增加。在常数β_(pol,PED)下,随着ν〜∗和/或中性气体注入的增加,观察到了宽度的进一步加宽,但尚不能排除原子物理效应对设置基座宽度的影响。单独的中性穿透并不能确定JET-ILW中边缘密度分布的形状。在实验不确定性范围内,边缘传输势垒区域中电子密度与电子温度标度长度之比η_e为2-3级。以静态线性剥离-气球模式稳定性和EPED基座结构模型表示的现有理解扩展到JET-ILW中ELM碰撞之间的动态演变,以测试这两个模型的基础假设。 JET-ILW中基座结构的ELM间时间演化不是唯一的,但取决于排放条件,例如加热功率和气体注入水平。随着在高功率下D _2气体注入的增加,p _(e,PED)的强烈减小主要是由于在ELM周期的一半夹住∇T _e,这表明湍流限制了T _e基座的生长。在低燃气率下,JET-ILW中的ELM基座间压力演化与EPED模型假设一致,而在高燃气率下,仅在低β情况下。在较高的贝塔系数和较高的气体速率下,ELM基座间的压力演化在质量上与动态膨胀模式(KBM)约束一致,但剥离-膨胀(P-B)约束未得到满足,并且ELM触发机制尚未解释。

著录项

  • 来源
    《Nuclear fusion》 |2017年第11期|116012.1-116012.15|共15页
  • 作者单位

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    Association VR, Fusion Plasma Physics, KTH, Stockholm, Sweden;

    Department of Physics, York Plasma Institute, University of York, York, United Kingdom;

    Department of Physics, York Plasma Institute, University of York, York, United Kingdom;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    Department of Physics, York Plasma Institute, University of York, York, United Kingdom;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    Department of Physics, York Plasma Institute, University of York, York, United Kingdom;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    National Institutes for QST, Naka, Japan;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

    Associação IST, Instituto Superior Técnico, Av Rovisco Pais, Lisbon, Portugal;

    CCFE, Culham Science Centre, Abingdon, United Kingdom;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    H-mode; inter-ELM pedestal evolution; JET-ILW; pedestal structure;

    机译:H模式ELM基座间的演变;JET-ILW;基座结构;
  • 入库时间 2022-08-18 00:41:37

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