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引用次数: 13
摘要
短电流脉冲在STOR‐M托卡马克(萨斯喀彻温环面修正)标称欧姆放电中的应用[物理学报]。流体[B], 3277(1992)]触发欧姆H模,其特征是Hα辐射减少,电子密度增加,边缘密度/磁波动减少。等离子体边缘和刮脱层的等离子体浮动电位测量表明,欧姆H模伴随着负等离子体自偏置,这导致边缘处的径向电场剖面更陡峭。由于电流脉冲持续时间(≤20 kA, 100 μsec)短于阻性趋肤时间(≂1 msec),因此可以预期边缘优先加热,这被认为是有利于诱发欧姆H模的边缘放电条件变化的原因。在H模式期间,电子密度分布在边缘处变得更陡峭,并且可以看到密度基座的清晰形成。密度分布的演化表明存在颗粒夹紧现象。一个改进的c…
Plasma autobiasing during Ohmic H‐mode in the STOR‐M tokamak
Application of a short current pulse on a nominal Ohmic discharge in the STOR‐M tokamak (Saskatchewan Torus‐Modified) [Phys. Fluids B 4, 3277 (1992)] triggers the Ohmic H‐mode characterized by reduced Hα radiation, increased electron density, and reduced edge density/magnetic fluctuations. Measurements of plasma floating potential at the plasma edge and in the scrape‐off layer indicate that the Ohmic H‐mode is accompanied by negative plasma autobiasing, which leads to a steeper radial electric field profile at the edge. Since the duration of the current pulse (≤20 kA, 100 μsec) is shorter than the resistive skin time (≂1 msec), preferential edge heating is expected, which is believed to be responsible for changes in the edge discharge condition favorable for inducing the Ohmic H‐mode. The electron density profile becomes steeper at the edge during the H‐mode, and clear formation of a density pedestal has been seen. The evolution of the density profile suggests the presence of particle pinch. An improved c...