射频鞘层驱动的边缘等离子体对流及其与H模式的相互作用

D. D'Ippolito, J. Myra, J. Jacquinot, M. Bureš
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引用次数: 66

摘要

研究表明,射频(rf)天线护套可以使边缘等离子体电位偏置,并在刮脱层(SOL)中驱动稳态对流细胞。由此产生的E×B对流流动与径向衰减玻姆鞘势引起的SOL中剪切流动的方向相反。二维流体模拟表明,当天线与等离子体的分离通常是天线处局部电子趋肤深度的几倍时,相反的极向流的相互作用产生了连接受限等离子体边缘和天线限制器的二次涡。对典型托卡马克边缘参数的估计表明,粒子和能量穿过这些漩涡的传递时间足够快,足以导致在单极相移中使用离子回旋加速器频率范围(ICRF)天线进行高功率加热时观察到的SOL密度和温度分布的扩大。射频鞘层驱动的对流也是解释相位依赖的一个很好的候选者。
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Radio‐frequency‐sheath‐driven edge plasma convection and interaction with the H mode
It is shown that radio‐frequency (rf) antenna sheaths can bias the edge plasma potential and drive steady‐state convective cells in the scrape‐off layer (SOL). The resulting E×B convective flow opposes the direction of the sheared flow in the SOL induced by the radially decaying Bohm sheath potential. A two‐dimensional fluid simulation shows that the interaction of the opposing poloidal flows produces secondary vortices, which connect the edge of the confined plasma to the antenna limiters, when the antenna–plasma separation is typically of order a few times the local electron skin depth at the antenna. Estimates for typical tokamak edge parameters suggest that the transit time of particles and energy across these vortices is rapid enough to cause the broadening of SOL density and temperature profiles observed during high‐power heating with ion cyclotron range of frequency (ICRF) antennas in monopole phasing. Radio‐frequency‐sheath‐driven convection is also a good candidate to explain the phasing dependen...
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