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Optimization of the safety factor profile for high noninductive current fraction discharges in DIII-D

机译:DIII-D中高无感电流分数放电的安全系数曲线的优化

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摘要

In order to assess the optimum q profile for discharges in DIII-D with 100% of the current driven noninductively (f_(NI) = 1), the self-consistent response of the plasma profiles to changes in the q profile was studied in high f_(NI), high β_N discharges through a scan of q_(min)and q_(95) at two values of β_N. As expected, both the bootstrap current fraction, f_(BS), and F_(NI) increased with q_(95). The temperature and density profiles were found to broaden as either q_(min) or β_N is increased. A consequence is that f_(BS) does not continue to increase at the highest values of q_(min). A scaling function that depends on q_(min),q_(95), and the peaking factor for the thermal pressure was found to represent well the f_(BS)/β_n inferred from the experimental profiles. The changes in the shapes of the density and temperature profiles as β_B is increased modify the bootstrap current density (J_(BS)) profile from peaked close to the axis to relatively flat in the region between the axis and the H-mode pedestal. Therefore, significant externally driven current density in the region inside the H-mode pedestal is required in addition to (J_(BS)) in order to match the profiles of the noninductive current density (J_(NI)) to the desired total current density (J). In this experiment, the additional current density was provided mostly by neutral beam current drive with the neutral-beam-driven current fraction 40-90% of f_(BS). The profiles of (J_(NI)) and J were most similar at q_(min)≈ 1.35-1.65,q95≈6.8, where f_(BS) is also maximum, establishing this q profile as the optimal choice for f_(NI) = 1 operation in DIII-D with the existing set of external current drive sources.
机译:为了评估DIII-D中100%无感驱动电流(f_(NI)= 1)时放电的最佳q分布图,研究了等离子体分布对q分布图变化的自洽响应f_(NI),高β_N通过对q_(min)和q_(95)的扫描以β_N的两个值放电。正如预期的那样,自举电流分数f_(BS)和F_(NI)都随q_(95)增大。发现温度和密度分布随q_(min)或β_N的增加而变宽。结果是,f_(BS)在q_(min)的最大值时不会继续增加。发现取决于q_(min),q_(95)的缩放函数以及热压的峰值因子可以很好地表示从实验曲线推断出的f_(BS)/β_n。随着β_B的增加,密度和温度分布图形状的变化将自举电流密度(J_(BS))分布图从接近轴峰的位置更改为在轴和H型基座之间的区域中相对平坦。因此,除了(J_(BS))之外,还需要H模式基座内部区域中的大量外部驱动电流密度,以使非感应电流密度(J_(NI))的分布与所需的总电流密度相匹配(J)。在此实验中,额外的电流密度主要由中性束电流驱动提供,其中中性束驱动的电流占f_(BS)的40-90%。 (J_(NI))和J的轮廓在q_(min)≈1.35-1.65,q95≈6.8时最相似,其中f_(BS)也是最大值,从而将此q轮廓确定为f_(NI)的最佳选择= DIII-D中使用现有一组外部电流驱动源进行的1次操作。

著录项

  • 来源
    《Nuclear fusion》 |2011年第6期|p.28.1-28.14|共14页
  • 作者单位

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    Lawrence Livermore National Laboratory, 700 East Ave, Livermore, CA 94550, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    Oak Ridge Institute for Science Education, Oak Ridge, TN 37830-8050, USA;

    Massachusetts Institute of Technology, 77 Massachusetts Ave, Cambridge, MA 02139, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    University of California-Los Angeles, PO Box 957099, Los Angeles, CA 90095-7099, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    Oak Ridge National Laboratory, PO Box 2008, Oak Ridge, TN 37831, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, USA;

    University of California-Los Angeles, PO Box 957099, Los Angeles, CA 90095-7099, USA;

    University of California-Los Angeles, PO Box 957099, Los Angeles, CA 90095-7099, USA;

  • 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
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  • 入库时间 2022-08-18 00:44:29

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