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FAST WAVE CURRENT DRIVE IN DIII-D

机译:DIII-D中的快速波电流驱动器

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The non-inductive current drive from fast Alfven waves launched by a directional four-element antenna was measured in the DIII-D tokamak. The fast wave frequency (60 MHz) was eight times the deuterium cyclotron frequency at the plasma center. An array of rf pickup loops at several locations around the torus was used to verify the directivity of the four-element antenna. Complete non-inductive current drive was achieved by using a combination of fast wave current drive (FWCD) and electron cyclotron current drive (ECCD) in discharges for which the total plasma current was inductively ramped down from 400 to 170 kA. For discharges with steady plasma current, up to 110 kA of FWCD was inferred from an alaysis of the loop voltage, with a maximum non-inductive current (FWCD, ECCD, and bootstrap) of 195 out of 310 kA. The FWCD efficiency increased linearly with the central electron temperature. For low current discharges, the FWCD efficiency was degraded because of incomplete fast wave damping. The experimental FWCD was found to agree with predictions from the CURRAY ray-tracing code only when a parasitic loss of 4% per pass was included in the modeling along with multiple pass damping.
机译:在DIII-D托卡马克中测量了由定向四元天线发射的快速Alfven波产生的非感应电流。快速波频率(60 MHz)是等离子体中心氘回旋加速器频率的八倍。在圆环周围多个位置的射频拾波环阵列用于验证四元件天线的方向性。通过在放电中使用快速波电流驱动(FWCD)和电子回旋加速器电流驱动(ECCD)的组合,可以实现完全的非感应电流驱动,为此,总等离子体电流感应地从400 kA下降到170 kA。对于具有稳定等离子电流的放电,从环路电压的分布可推断出高达110 kA的FWCD,而在310 kA中,最大非感应电流(FWCD,ECCD和自举)为195。 FWCD效率随中心电子温度线性增加。对于低电流放电,由于不完整的快速波阻尼,FWCD效率降低了。仅在建模中将每通道4%的寄生损耗与多通道阻尼一起包括在内时,发现实验FWCD与CURRAY射线跟踪代码的预测一致。

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