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Parametric study of two-dimensional potential structures induced by radio-frequency sheaths coupled with transverse currents in front of the Ion Cyclotron Resonance Heating antenna

机译:离子回旋共振加热天线前射频鞘管与横向电流耦合产生的二维势结构的参数研究

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For the first time, a two-dimensional (2D) fluid model and an analytical expression for the rectified potential with respect to the transverse polarization current are established and verified by a 2D PIC (particle in cell) code over the validity domain of our model. Then the model is extended to the overall ion cyclotron frequency range used in different heating and current drive scenarios. First, the models demonstrate that these transverse polarization currents add some inertia in the temporal dynamic. Due to the nonlinear behavior of the I-V sheath characteristic, the time average amplitude (dc potential) of the rectified potential structure is increased compared to the time average rf potential. Second, they induce only a slight widening of the potential structure. Such modifications are quantified using a "test map" initially characterized by a Gaussian shape. The map is assumed to remain Gaussian near its summit. The time behavior of the peak can be estimated analytically in the presence of polarization current as a function of its width r(0) and amplitude phi(0) (normalized to local temperature and to a characteristic length for transverse transport). A potential peaking criterion has been built to determine the peaking zone of the dc potential structure induced by the rf field. Computations made for typical parameters of the edge plasma in front of the antenna of the Tokamak Tore Supra show that the dc rectified potential is up to 50% higher than the previous computations neglecting polarization current effects. The weak diffused and high dc potential structures computed can explain the hot spot formation induced by convective cells associated to high energetic ion fluxes on the corners of the Ion Cyclotron Resonance Heating antenna. (c) 2006 American Institute of Physics.
机译:首次建立二维(2D)流体模型和相对于横向极化电流的整流电势的解析表达式,并在模型的有效范围内通过2D PIC(单元中的粒子)代码进行了验证。然后,将模型扩展到在不同加热和电流驱动方案中使用的总离子回旋加速器频率范围。首先,模型证明这些横向极化电流在时间动态中增加了一些惯性。由于I-V护套特性的非线性行为,整流后的电势结构的时间平均幅度(直流电势)与时间平均rf电势相比有所增加。其次,它们仅引起潜在结构的轻微扩展。使用最初以高斯形状为特征的“测试图”来量化这种修改。假定该地图在其山顶附近仍保持高斯状态。在存在极化电流的情况下,可以根据其宽度r(0)和振幅phi(0)(针对局部温度和横向传输的特征长度进行归一化),通过解析估算峰的时间行为。已经建立了一个电位峰值准则来确定由rf场感应的dc电位结构的峰值区域。对Tokamak Tore Supra天线前面的边缘等离子体的典型参数进行的计算表明,直流整流电势比忽略极化电流影响的先前计算高出50%。计算得到的弱扩散和高直流电势结构可以解释由对流电池引起的热点形成,该对流电池与离子回旋加速器共振加热天线角上的高能离子通量有关。 (c)2006年美国物理研究所。

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