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Non-linear MHD modelling of edge localized modes dynamics in KSTAR

机译:KSTAR中边缘局部模式动力学的非线性MHD建模

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摘要

The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge localized mode (ELM) crash and in the inter-ELM periods (ELM precursors) observed in KSTAR is provided for the first time in the present paper. The dynamics of ELMs, observed using electron cyclotron emission imaging (ECEI) in KSTAR tokamak, is compared to the modelling results of the non-linear reduced resistive MHD code JOREK. The realistic KSTAR pulse parameters and geometry including X-point and scrape off layer (SOL) were used. The full ELM crash modelling was performed using JOREK code for single and multi-harmonic representation and in multi-cycles ELMy regimes including relevant flows. The most unstable toroidal modes numbers (n = 5-8), velocity (~5 km s~(-1) for n = 8 mode) and the direction of the mode rotation were reproduced in modelling. The two fluid diamagnetic effects and toroidal rotations included in the model were found to be the most important factors in explaining the experimentally observed rotation of the ballooning modes before the ELM crash and in the inter-ELM phase. In multi-harmonic multi-cycle simulations the spectrum of temperature fluctuations is similar to the experimental one in the inter-ELM phase, where several rotating modes with medium n numbers were detected in 5-30 kHz frequency range. The rotating modes can contain single or several harmonics which last from 0.2 ms to few ms in time, and can appear and disappear in the inter ELM period or persist until a new ELM crash.
机译:本文首次解释了在I型边缘局域模式(ELM)崩溃之前的基座区域以及在KSTAR中观测到的ELM间周期(ELM前驱体)中旋转MHD模式的存在。使用电子回旋加速器发射成像(ECEI)在KSTAR托卡马克中观察到的ELM的动力学与非线性降阻MHD代码JOREK的建模结果进行了比较。使用了实际的KSTAR脉冲参数和几何形状,包括X点和刮擦层(SOL)。完整的ELM崩溃建模是使用JOREK代码进行的单次和多次谐波表示,以及在包括相关流程在内的多周期ELMy机制中执行的。在建模中复制了最不稳定的环形模式编号(n = 5-8),速度(对于n = 8模式为〜5 km s〜(-1))和模式旋转方向。发现在模型中包括的两个流体抗磁效应和环形旋转是解释实验观察到的在ELM碰撞之前和在ELM间阶段的膨胀模式旋转的最重要因素。在多谐波多周期仿真中,温度波动的频谱类似于在ELM间阶段的实验,其中在5-30 kHz频率范围内检测到数个中等n数的旋转模式。旋转模式可以包含单次或多次谐波,其持续时间从0.2毫秒到几毫秒,并且可以在ELM间隔期间出现和消失,或者持续到新的ELM崩溃为止。

著录项

  • 来源
    《Nuclear fusion》 |2017年第11期|116059.1-116059.12|共12页
  • 作者单位

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France;

    Ulsan National Institute of Science and Technology (UNIST), 44919, Ulsan, Republic of Korea;

    Pohang University of Science and Technology, Pohang, Gyeongbuk 790-784, Republic of Korea;

    CCFE, Culham Science Centre, Oxon, 0X14 3DB, Abingdon, United Kingdom;

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France;

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France;

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France,Eindhoven University of Technology, Eindhoven, Netherlands;

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France;

    CEA, IRFM, 13108 Saint-Paul-Lez-Durance, France;

    Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany;

    Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany;

    Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching, Germany;

  • 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

    ELM; KSTAR; ECEI; rotation; ballooning modes; diamagnetic; resistive non-linear MHD; modelling; inter ELM-period; precursors;

    机译:榆树;科士达;ECEI;回转;膨胀模式;抗磁性电阻非线性MHD;造型;跨ELM期间;前体;
  • 入库时间 2022-08-18 00:41:39

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