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The effect of diamagnetic drift on the boundary conditions in tokamak scrape-off layers and the distribution of plasma fluxes near the target

机译:抗磁漂移对托卡马克刮除层边界条件的影响及靶区附近等离子体通量分布

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The standard model for the two-dimensional simulation of the scrape-off layer (SOL) in the divertor is based on the equations for anomalous cross-field particle and energy transport and classical parallel transport. Recently, it has been complemented by the fluid equations of Braginskii to include all classical fluxes in a self-consistent way. The main physical effect of introducing classical fluxes is the appearance of two new terms-an electrical E*B drift and a diamagnetic B* Del P drift, as well as B* Del T contributions to the energy transport. Although the new models provide an adequate consideration of all the classical fluxes inside the plasma, a mistake has typically been made in the literature in formulating the new boundary conditions. The poloidal component of the B* Del Pidrift, existing inside the plasma, is assumed to continue through to the target surface, thus altering the Bohm criterion. Likewise, the poloidal current due to the B* Del (Pi+Pe) term is assumed to reach the surface, changing the surface electric potential drop. In this paper we demonstrate, however, that the diamagnetic fluxes in the whole plasma, including the SOL region, in their major part can be represented by the curl of a vector and, therefore, are self-terminating. We have made a detailed analysis of the distribution of plasma pressure and fluxes at the boundary between the plasma and the surface, encompassing the magnetic presheath and Debye sheath layers. After entering the presheath entrance, the poloidal component of the diamagnetic flux is diverted in the direction along the material surface due to the sharp pressure gradient in the presheath region. This creates boundary drift flows along the surface. Because of that conversion of the poloidal diamagnetic fluxes into boundary fluxes they do not deliver particles and current to the surface and therefore must not be included in the modified boundary conditions. Kinetic analysis of the distribution of the fluxes near the target also reveals an additional ExB drift in the radial direction, which mainly affects the ion motion in the magnetic presheath and Debye sheath layers. This drift is expected to shift the density profile of the plasma near the target in the radial direction a distance of the order of the ion poloidal Larmor radius.
机译:分流器中刮掉层 (SOL) 二维模拟的标准模型基于异常跨场粒子和能量传输以及经典平行传输的方程。最近,它得到了Braginskii流体方程的补充,以自洽的方式包括所有经典通量。引入经典通量的主要物理效应是出现了两个新术语——电 E*B 漂移和抗磁性 B* Del P 漂移,以及 B* Del T 对能量传递的贡献。尽管新模型充分考虑了等离子体内部的所有经典通量,但在制定新的边界条件时,文献中通常会犯一个错误。假设存在于等离子体内部的 B* Del Pidrift 的极化分量继续延伸到目标表面,从而改变了 Bohm 准则。同样,假设由于 B* Del (Pi+Pe) 项引起的极化电流到达表面,从而改变表面电势降。然而,在本文中,我们证明了整个等离子体(包括 SOL 区域)中的抗磁通量在其主要部分可以用矢量的卷曲来表示,因此是自终止的。我们对等离子体和表面边界处等离子体压力和通量的分布进行了详细分析,包括磁性预护套和德拜护套层。进入预护套入口后,由于预护套区域的急剧压力梯度,抗磁通量的极化分量沿材料表面方向转移。这将沿表面产生边界漂移流。由于极化抗磁通量转换为边界通量,因此它们不会将粒子和电流输送到表面,因此不得包含在修改后的边界条件中。对靶材附近通量分布的动力学分析还揭示了径向上的额外ExB漂移,这主要影响磁性预护套和德拜护套层中的离子运动。预计这种漂移会使目标附近等离子体的密度分布在径向上移动离子极化拉莫尔半径的距离。

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