从轴向-径向动力学模型看非麦克斯韦电子对霍尔推进器放电宏观响应的影响

A. Marín-Cebrián, E. Bello-Benítez, A. Domínguez-Vázquez, E. Ahedo
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摘要

我们建立了霍尔推进器放电的二维轴向-径向 "粒子-单元"(PIC)模型,(主要)分析电子方位平均慢速动力学所满足的流体方程。电子的弱碰撞性以及与推进器壁的强相互作用导致了非麦克斯韦速度分布函数(VDF)。因此,所产生的宏观响应不同于传统的碰撞流体。首先,压力张量的回旋(对角线)部分是各向异性的。其次,它的回旋部分虽然很小,但在方位动量平衡中很重要,其主要贡献比轴向动量平衡低几个数量级。第三,热通量矢量并不满足简单的定律,尽管可以分别确定平行和垂直分量的对流和传导行为。第四,电子壁相互作用参数在很大程度上不同于基于近似麦克斯韦 VDF 的经典鞘理论。此外,这些效应在通道的近阳极和近出口区域的表现也不同。不过,基本等离子体幅值的剖面与一维轴向流体模型的剖面非常吻合。为了便于解释等离子体的响应,我们使用了准平面几何、纯径向磁场和简单的交叉磁场传输经验模型;但也可以加入现实配置和更复杂的反常扩散公式。通过使用增强的真空介电常数和中性静止耗尽定律来控制计算时间。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Non-Maxwellian electron effects on the macroscopic response of a Hall thruster discharge from an axial-radial kinetic model
A 2D axial-radial particle-in-cell (PIC) model of a Hall thruster discharge has been developed to analyze (mainly) the fluid equations satisfied by the azimuthally-averaged slow dynamics of electrons. Their weak collisionality together with a strong interaction with the thruster walls lead to a non-Maxwellian velocity distribution function (VDF). Consequently, the resulting macroscopic response differs from a conventional collisional fluid. First, the gyrotropic (diagonal) part of the pressure tensor is anisotropic. Second, its gyroviscous part, although small, is relevant in the azimuthal momentum balance, where the dominant contributions are orders of magnitude lower than in the axial momentum balance. Third, the heat flux vector does not satisfy simple laws, although convective and conductive behaviors can be identified for the parallel and perpendicular components, respectively. And fourth, the electron wall interaction parameters can differ largely from the classical sheath theory, based on near Maxwellian VDF. Furthermore, these effects behave differently in the near-anode and near-exit regions of the channel. Still, the profiles of basic plasma magnitudes agree well with those of 1D axial fluid models. To facilitate the interpretation of the plasma response, a quasiplanar geometry, a purely-radial magnetic field, and a simple empirical model of cross-field transport were used; but realistic configurations and a more elaborated anomalous diffusion formulation can be incorporated. Computational time was controlled by using an augmented vacuum permittivity and a stationary depletion law for neutrals.
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