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Full kinetic simulations of plasma flow interactions with meso- and microscale magnetic dipoles

机译:等离子体流与中微尺度磁偶极子相互作用的全动力学模拟

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摘要

We examined the plasma flow response to meso- and microscale magnetic dipoles by performing three-dimensional full particle-in-cell simulations. We particularly focused on the formation of a magnetosphere and its dependence on the intensity of the magnetic moment. The size of a magnetic dipole immersed in a plasma flow can be characterized by a distance L from the dipole center to the position where the pressure of the local magnetic field becomes equal to the dynamic pressure of the plasma flow under the magnetohydrodynamics (MHD) approximation. In this study, we are interested in a magnetic dipole whose L is smaller than the Larmor radius of ions r(iL) calculated with the unperturbed dipole field at the distance L from the center. In the simulation results, we confirmed the clear formation of a magnetosphere consisting of a magnetopause and a tail region in the density profile, although the spatial scale is much smaller than the MHD scale. One of the important findings in this study is that the spatial profiles of the plasma density as well as the current flows are remarkably affected by the finite Larmor radius effect of the plasma flow, which is different from the Earth's magnetosphere. The magnetopause found in the upstream region is located at a position much closer to the dipole center than L. In the equatorial plane, we also found an asymmetric density profile with respect to the plasma flow direction, which is caused by plasma gyration in the dipole field region. The ion current layers are created in the inner region of the dipole field, and the electron current also flows in the region beyond the ion current layer because ions with a large inertia can closely approach the dipole center. Unlike the ring current structure of the Earth's magnetosphere, the current layers in the microscale dipole fields are not circularly closed around the dipole center. Since the major current is caused by the particle gyrations, the current is independently determined to be in the direction of the electron and ion gyrations, which are the same in both the upstream and downstream regions. The present analysis on the formation of a magnetosphere in the regime of a microscale magnetic dipole is significant for understanding the solar wind response to the crustal magnetic anomalies on the Moon surface, such as were recently observed by spacecraft. (C) 2014 AIP Publishing LLC.
机译:我们通过执行三维全粒子模拟,检查了等离子体流对中微尺度磁偶极子的响应。我们特别关注磁层的形成及其对磁矩强度的依赖性。浸没在等离子体流中的磁偶极子的大小可以用偶极子中心到在磁流体动力学(MHD)近似下局部磁场的压力等于等离子体流的动压力的位置的距离L来表征。 。在这项研究中,我们对一个磁偶极子感兴趣,该偶极子的L小于在离中心距离L处用不受干扰的偶极子场计算出的离子的拉莫尔半径r(iL)。在模拟结果中,尽管空间尺度远小于MHD尺度,但我们确认了磁层的清晰形成,该磁层由磁层顶和尾部区域组成。这项研究的重要发现之一是,等离子流的有限拉莫尔半径效应显着影响了等离子密度和电流的空间分布,这与地球的磁层不同。在上游区域发现的磁绝顶位于比L更靠近偶极中心的位置。在赤道平面中,我们还发现了相对于等离子体流动方向的不对称密度分布,这是由偶极中的等离子体回旋引起的现场区域。在偶极场的内部区域中产生离子电流层,并且电子电流也流过离子电流层以外的区域,因为具有大惯性的离子可以紧密接近偶极中心。与地球磁层的环形电流结构不同,微尺度偶极子场中的电流层在偶极子中心周围不是圆形封闭的。由于主要电流是由粒子旋转引起的,因此电流独立确定为沿电子和离子旋转的方向,在上游和下游区域都相同。目前在微尺度磁偶极子状态下形成磁层的分析对于理解太阳风对月球表面地壳磁异常的响应具有重要意义,例如最近由航天器观测到的。 (C)2014 AIP Publishing LLC。

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