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首页> 外文期刊>Nuclear fusion >Characterization of broadband MHD fluctuations during type-Ⅱ edge localized modes as measured in 2D with ECE-imaging at ASDEX Upgrade
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Characterization of broadband MHD fluctuations during type-Ⅱ edge localized modes as measured in 2D with ECE-imaging at ASDEX Upgrade

机译:在ASDEX升级中使用ECE成像在2D模式下测量的II型边缘局域模式中宽带MHD波动的特征

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摘要

The characterization of a broadband fluctuation that is typical for the type-Ⅱ ELM regime at ASDEX Upgrade has been improved using the 2D capabilities of ECE-imaging. During the transition from the type-Ⅰ to type-Ⅱ ELMy phase, it has been found that electron temperature fluctuations form a broadband peak in the 19-65 kHz range. In the type-Ⅱ phase, this broadband fluctuation reaches a maximum relative amplitude of almost 20% just inside the top of the pedestal. Simultaneously, the electron temperature profile is completely flattened at this location. The 2D distribution of the amplitude of this broadband fluctuation is such that, when averaged over time, a minimum occurs around the mid-plane. From the measurements of the nearby magnetic pickup coils, a similar broadband fluctuation seems visible in the same frequency range. However, this is peaked at a slightly lower frequency and does not show a similar minimum. From the analysis of the fluctuations on small timescales, the poloidal and toroidal mode numbers are estimated to be m ~ 100 and n ~ 21. Furthermore, activity reminiscent of beat waves has been observed, which might partially account for the fluctuation's broadband nature and the seeming velocity variation of single fluctuation passages. Overall, similarities between the characteristics of this broadband fluctuation and various precursors to type-Ⅰ ELMs suggest that this fluctuation can play an important role in regulating the ELM cycle.
机译:通过使用ECE成像的2D功能,改进了ASDEX升级时II型ELM机制典型的宽带波动特征。从Ⅰ型到Ⅱ型ELMy相的转变过程中,已经发现电子温度波动在19-65 kHz范围内形成一个宽带峰。在Ⅱ型阶段,该宽带波动恰好在基座顶部内部达到了近20%的最大相对幅度。同时,电子温度曲线在该位置完全变平。该宽带波动幅度的2D分布是这样的:当对时间进行平均时,在中平面附近会出现最小值。从附近磁性拾波器线圈的测量结果来看,在相同频率范围内,可见到类似的宽带波动。但是,它在稍低的频率处达到峰值,并且没有显示相似的最小值。从小时间尺度上的波动分析来看,估计的极坐标和环形模数分别为m〜100和n〜21。此外,还观察到了拍频波的活动,这可能部分解释了波动的宽带性质和单个波动通道的表面速度变化。总体而言,这种宽带波动的特征与Ⅰ型ELM的各种前兆之间的相似性表明,这种波动可以在调节ELM周期中发挥重要作用。

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  • 来源
    《Nuclear fusion》 |2012年第11期|114004.1-114004.8|共8页
  • 作者单位

    FOM Institute DIFFER - Dutch Institute for Fundamental Energy Research, Association EURATOM-FOM, 3430 BE Nieuwegein, The Netherlands;

    Max-Planck-Institut fuer Plasmaphysik, 85748 Garching bei Muenchen, Germany;

    FOM Institute DIFFER - Dutch Institute for Fundamental Energy Research, Association EURATOM-FOM, 3430 BE Nieuwegein, The Netherlands;

    FOM Institute DIFFER - Dutch Institute for Fundamental Energy Research, Association EURATOM-FOM, 3430 BE Nieuwegein, The Netherlands;

    Max-Planck-Institut fuer Plasmaphysik, 85748 Garching bei Muenchen, Germany;

    Max-Planck-Institut fuer Plasmaphysik, 85748 Garching bei Muenchen, Germany;

    Max-Planck-Institut fuer Plasmaphysik, 85748 Garching bei Muenchen, Germany;

    FOM Institute DIFFER - Dutch Institute for Fundamental Energy Research, Association EURATOM-FOM, 3430 BE Nieuwegein, The Netherlands,Faculteit Technische Natuurkunde, Technische Universiteit Eindhoven, 5600 MB Eindhoven, The Netherlands;

    Princeton Plasma Physics Laboratory, Princeton, NJ 08540, USA;

    Department of Electrical and Computer Engineering, University of California at Davis, Davis, CA 95616, USA;

    Department of Electrical and Computer Engineering, University of California at Davis, Davis, CA 95616, USA;

    POSTECH, Pohang, Gyeongbuk, 790-784, Korea;

  • 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);
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