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Effect of poloidal phasing on ion cyclotron resonance heating power absorption

机译:极性定相对离子回旋共振加热功率吸收的影响

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摘要

Two ion cyclotron resonance heating (ICRH) systems are planned for ITER, each system containing 24 antennas distributed as a two by four array of poloidal triplets. The ITER antennas are designed to operate at a poloidal phase difference between the upper and lower triplet of Delta theta(pol) = +/- 90 degrees in the antenna currents. Since current tokamak experiments normally operate at Delta theta(pol) = 0 degrees, experience from ICRH schemes with Delta theta(pol) not equal 0 is lacking. In this paper, the effects of poloidal phasing on ICRH power absorption and coupling are studied using the novel code FEMIC, which is described here. Simulations of the ITER antenna and the JET ITER-like antenna show that increasing the poloidal phase difference increases the destructive interference of the fast magnetosonic wave near the equatorial plane. This causes a degradation of the on-axis heating performance and reduces the total coupled power to the plasma. Best on-axis heating was obtained for Delta theta(pol) = 0 degrees, resulting in peaked profiles. By increasing the poloidal phase difference the absorption profiles tend to become less peaked or hollow on-axis. The effect is localized and occurs for rho(pol) less than or similar to 0.1, i.e. near the magnetic axis. The total coupled power was found to be asymmetric around Delta theta(pol) = 0 degrees due to the plasma gyrotropy, where the maximum coupled power occurs within -33 degrees less than or similar to Delta theta(pol) less than or similar to - 22 degrees on ITER and JET. The exact location of the maximum depends on the width of the pedestal. The strength of the asymmetry increases with the pedestal width.
机译:计划为ITER设计两个离子回旋共振加热(IC​​RH)系统,每个系统包含24个天线,这些天线以两乘四列的三倍体阵列分布。 ITER天线被设计为在天线电流中Delta theta(pol)= +/- 90度的上下三重态之间的倍体相位差下工作。由于当前的托卡马克实验通常在Delta theta(pol)= 0度下运行,因此缺少来自ICRH方案的Delta theta(pol)不等于0的经验。在本文中,使用新颖的代码FEMIC研究了倍相调相对ICRH功率吸收和耦合的影响,在此进行描述。对ITER天线和类似JET的JET天线的仿真表明,增加倍数相差会增加赤道面附近快速磁声波的破坏性干扰。这导致同轴加热性能的下降,并降低了与等离子体的总耦合功率。对于Delta theta(pol)= 0度,可获得最佳的同轴加热,从而导致峰值轮廓。通过增加倍体相差,吸收曲线趋向于变得不那么尖峰或同轴。该效应是局部的,并且对于rho(pol)小于或类似于0.1,即在磁轴附近发生。由于等离子回旋,总耦合功率在Δtheta(pol)= 0度附近是不对称的,其中最大耦合功率出现在小于或类似于-33度的Delta theta(pol)小于或类似于-在ITER和JET上为22度。最大值的确切位置取决于基座的宽度。不对称强度随基座宽度的增加而增加。

著录项

  • 来源
    《Nuclear fusion》 |2019年第7期|076022.1-076022.15|共15页
  • 作者单位

    KTH, Dept Fus Plasma Phys, Sch Elect Engn & Comp Sci, SE-10044 Stockholm, Sweden;

    KTH, Dept Fus Plasma Phys, Sch Elect Engn & Comp Sci, SE-10044 Stockholm, Sweden;

    LPP ERM KMS, Lab Plasma Phys, B-1000 Brussels, Belgium;

    KTH, Dept Fus Plasma Phys, Sch Elect Engn & Comp Sci, SE-10044 Stockholm, Sweden;

    KTH, Dept Fus Plasma Phys, Sch Elect Engn & Comp Sci, SE-10044 Stockholm, Sweden;

  • 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

    poloidal phasing; ICRH; ITER; FEMIC;

    机译:极性定相;ICRH;ITER;FEMIC;
  • 入库时间 2022-08-18 04:20:08

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