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Quasi-steady State High Confinement at High Density by LH Waves in the HT-6M Tokamak

机译:HT-6M托卡马克中LH波高密度准稳态高密闭

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The quasi-steady-state (t_H> 10_(τEoh)) H-mode with high plasma density (ELMy and ELMy free) wasrnroutinely obtained by the injection of Lower Hybrid Heating (LHH) and Lower Hybrid Current Drive (LHCD) withrna power threshold of 50 kW . The antenna spectrum was scanned in wide range and tE was about 1.5~2.0 times ofrnthe L-mode scaling. The density increases almost three times during the H-phase by gas puffing and the particlernconfinement time increases more than two times even with a line average density of 3×10~(13)cm~(-3) , which is about 60%rnthe Greenwald density limit. A hollow T_e profile was achieved in the high density case. The experimental resultsrnreproducibly show a good agreement with the theoretical prediction for the LH off-axis power deposition profile.rnWhen a certain of fraction of the plasma current is non-inductively sustained by the LH waves, a hollow currentrndensity profile is formed and the magnetic shear is reversed. This off-axis hollow current profile and enhancedrnconfinement improvement are attributed to a strong reduction of electron thermal diffusivity in the reversed shearrnregion.
机译:通过注入具有低功率阈值的低混合加热(LHH)和低混合电流驱动(LHCD)常规获得具有高等离子体密度(ELMy和ELMy自由)的准稳态(t_H> 10_(τEoh))H模式50千瓦。在大范围内扫描天线频谱,tE约为L模式缩放的1.5〜2.0倍。在H相中,通过吹气,密度几乎增加了三倍,并且即使线平均密度为3×10〜(13)cm〜(-3),粒子约束时间也增加了两倍以上,约为60%。格林瓦尔德密度极限。在高密度情况下获得了空心的T_e轮廓。实验结果可重复地显示出与LH离轴功率沉积轮廓的理论预测吻合良好.rn当LH波非感应地维持一定比例的等离子体电流时,会形成空心电流rn轮廓并产生磁剪切是相反的。这种偏轴空心电流分布和增强的约束效果归因于反向剪切区域中电子热扩散率的极大降低。

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  • 来源
    《Fusion energy 1998》|1998年|p.1-4|共4页
  • 会议地点 Yokohama(JP)
  • 作者单位

    Institute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

    rnInstitute of Plasma Physics, Academia Sinica, 230031, Hefei, P.R.China;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 受控热核反应(聚变反应理论及实验装置);
  • 关键词

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