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Observations of fast anisotropic ion heating, ion cooling, and ion recycling in large-amplitude drift waves

机译:大振幅漂移波中快速各向异性离子加热,离子冷却和离子回收的观察

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摘要

Large-amplitude drift wave fluctuations are observed to cause severe ion temperature oscillations in plasmas of the Caltech Encore tokamak [J. M. McChesney, P. M. Bellan, and R. A. Stern, Phys. Fluids B 3, 3370 (1991)]. Experimental investigations of the complete ion dynamical behavior in these waves are presented. The wave electric field excites stochastic ion orbits in the plane normal (perpendicular to) to B, resulting in rapid perpendicular to heating. Ion-ion collisions impart energy along (parallel to) B, relaxing the perpendicular to-parallel to temperature anisotropy. Hot ions with large orbit radii escape confinement, reaching the chamber wall and cooling the distribution. Cold ions from the plasma edge convect back into the plasma (i.e., recycle), causing further cooling and significantly replenishing the density depleted by orbit losses. The ion-ion collision period tau(ii)similar to Tau(3/2)/n fluctuates strongly with the drift wave phase, due to intense (approximate to 50%) fluctuations in n and Tau. Evidence for particle recycling is given by observations of bimodal ion velocity distributions near the plasma edge, indicating the presence of cold ions (0.4 eV) superposed atop the hot (4-8 eV) plasma background. These appear periodically, synchronous with the drift wave phase at which ion fluid flow from the wall toward the plasma center peaks. Evidence is presented that such a periodic heat/loss/recycle/cool process is expected in plasmas with strong stochastic heating.
机译:观察到大振幅的漂移波波动会在Caltech Encore托卡马克等离子体中引起严重的离子温度振荡[J. M. McChesney,P.M。Bellan和R.A. Stern,物理学流体B 3,3370(1991)]。提出了在这些波中完成离子动力学行为的实验研究。波电场激发垂直于B平面(垂直于B平面)的随机离子轨道,从而迅速垂直于加热。离子碰撞沿着(平行于)B传递能量,从而放松了垂直于平行于温度各向异性的方向。具有大轨道半径的热离子逃逸封闭,到达室壁并冷却分布。来自等离子体边缘的冷离子对流回到等离子体中(即,再循环),引起进一步的冷却并显着补充由轨道损耗所耗尽的密度。由于n和Tau的剧烈波动(约50%),类似于Tau(3/2)/ n的离子-离子碰撞周期tau(ii)随漂移波相位而剧烈波动。通过观察等离子体边缘附近的双峰离子速度分布可以得出粒子回收的证据,表明存在冷离子(0.4 eV)叠加在热(4-8 eV)等离子体背景上。这些与漂移波相位同步出现,在该漂移波相位处,离子流体从壁流向等离子体中心达到峰值。证据表明,在具有强烈随机加热的等离子体中,预期会出现这种周期性的热/损失/循环/冷却过程。

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