P. G. Matthews, David L. T. Anderson, F. Anderson, J. Shohet, J. Talmadge
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引用次数: 10
摘要
在可互换模块仿星器(IMS)上对二维等离子体横截面的平均和波动密度、电子温度、电势以及雷诺应力进行了探针测量[D]。T. Anderson, J. A. Derr, J. L. Shohet, IEEE译。等离子体科学。[j].生物工程学报,2012(1)。这些测量是在两种磁场强度下进行的,也是在正偏置电极诱导极向等离子体流时进行的。数据表明,波动诱导的输运是极性不对称的,并且依赖于电子回旋共振位置的位置和电极偏置。诱导极向等离子体流通过改变密度和势振荡的相位关系,将名义上的向外波动诱导的粒子输运转变为向内(负径向输运)。一般来说,密度和电位波动的振幅不会因剪切的极向流而减小。将计算得到的雷诺应力诱导的极向等离子体流与动量平衡计算得到的极向等离子体流进行了比较。
Fluctuation-induced transport and poloidal rotation in the interchangeable module stellarator
Probe measurements over the two‐dimensional plasma cross section of the average and fluctuating density, electron temperature, and potential, as well as the Reynolds stress, have been made in the Interchangeable Module Stellarator (IMS) [D. T. Anderson, J. A. Derr, and J. L. Shohet, IEEE Trans. Plasma Sci. PS‐9, 212 (1981)]. These measurements were performed at two magnetic field strengths, and also when a positively biased electrode induces a poloidal plasma flow. The data shows the fluctuation‐induced transport to be poloidally asymmetric and dependent upon the location of the electron cyclotron resonance position, and upon the electrode biasing. The induced poloidal plasma flow changes the nominally outward fluctuation‐induced particle transport to be inward (negative radial transport) by changing the phase relationship of the density and potential oscillations. The amplitude of the density and potential fluctuations are, in general, not reduced by the sheared poloidal flow. Calculations are presented comparing the computed Reynolds stress induced poloidal plasma flows with the flow calculated from momentum balance.