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arXiv 1907.08482physics.plasm-ph
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主离子压力各向异性对仿星器杂质输运的影响

Impact of main ion pressure anisotropy on stellarator impurity transport

Ivan Calvo, Felix I. Parra, J. L. Velasco, J. M. García-Regaña

摘要:

主离子通过各种机制影响杂质动力学,特别是通过杂质离子碰撞。对于主离子质量相对于杂质质量的展开式中的最低阶,杂质-离子碰撞算符仅依赖于主离子分布中平行速度为奇数的分量。这些最低阶项给出了杂质与主离子的平行摩擦,这通常被认为是碰撞杂质输运的主要原因。杂质离子碰撞算子的质量比展开中的次阶项,与平行速度中的主离子分布的分量成比例,通常被忽略。然而,在仿星器中,主离子分布的均匀分量可能非常大。本文保留了杂质-离子碰撞算符质量比展开式中的次一阶项,并计算了Pfirsch-Schlüter、plateau和$1/ν$区中痕量杂质的新经典径向通量的解析表达式.新的术语提供了一种杂质传输的驱动力,这种驱动力在物理上与平行摩擦非常不同:它们与主离子压力的各向异性有关,而主离子压力的各向异性又转化为杂质压力的各向异性。有人认为,主离子压力的各向异性必须考虑到在某些现实仿星器等离子体中的杂质输运的正确描述。通过数值计算给出了杂质通量的解析表达式。

英文摘要:

Main ions influence impurity dynamics through a variety of mechanisms; in particular, via impurity-ion collisions. To lowest order in an expansion in the main ion mass over the impurity mass, the impurity-ion collision operator only depends on the component of the main ion distribution that is odd in the parallel velocity. These lowest order terms give the parallel friction of the impurities with the main ions, which is typically assumed to be the main cause of collisional impurity transport. Next-order terms in the mass ratio expansion of the impurity-ion collision operator, proportional to the component of the main ion distribution that is even in the parallel velocity, are usually neglected. However, in stellarators, the even component of the main ion distribution can be very large. In this article, such next-order terms in the mass ratio expansion of the impurity-ion collision operator are retained, and analytical expressions for the neoclassical radial flux of trace impurities are calculated in the Pfirsch-Schlüter, plateau and $1/ν$ regimes. The new terms provide a drive for impurity transport that is physically very different from parallel friction: they are associated to anisotropy in the pressure of the main ions, which translates into impurity pressure anisotropy. It is argued that main ion pressure anisotropy must be taken into account for a correct description of impurity transport in certain realistic stellarator plasmas. Examples are given by numerically evaluating the analytical expressions for the impurity flux.

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