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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Dynamic Harris current sheet thickness from Cluster current density and plasma measurements
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Dynamic Harris current sheet thickness from Cluster current density and plasma measurements

机译:哈里斯动态电流片厚度集群电流密度和等离子体测量

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We use the first accurate measurements of current densities in the plasma sheet to calculate the half-thickness and position of the current sheet as a function of time. Our technique assumes a Harris current sheet model, which is parameterized by lobe magnetic field B 0, current sheet half-thickness h, and current sheet position z 0. Cluster measurements of magnetic field, current density, and plasma pressure are used to infer the three parameters as a function of time. We find that most long timescale (6–12 hours) current sheet crossings observed by Cluster cannot be described by a static Harris current sheet with a single set of parameters B 0, h, and z 0. Noting the presence of high-frequency fluctuations that appear to be superimposed on lower frequency variations, we average over running 6-min intervals and use the smoothed data to infer the parameters h(t) and z 0(t), constrained by the pressure balance lobe magnetic field B 0(t). Whereas this approach has been used in previous studies, the spatial gradients now provided by the Cluster magnetometers were unavailable or not well constrained in earlier studies. We place the calculated half-thicknesses in a magnetospheric context by examining the change in thickness with substorm phase for three case study events and 21 events in a superposed epoch analysis. We find that the inferred half-thickness in many cases reflects the nominal changes experienced by the plasma sheet during substorms (i.e., thinning during growth phase, thickening following substorm onset). We conclude with an analysis of the relative contribution of ?B Z /?X to the cross-tail current density during substorms. We find that ?B Z /?X can contribute a significant portion of the cross-tail current around substorm onset.
机译:我们使用的第一个准确的测量电流等离子体的密度表计算half-thickness和当前表的位置作为时间的函数。哈里斯当前表模型,这是参数化叶磁场B 0,电流表half-thickness h,和当前表z位置0。场、电流密度和等离子体的压力用来推断三个参数的函数的时间。小时)电流片交叉观测到集群不能由一个静态描述哈里斯当前表使用一组参数B0, h, z 0。高频波动,似乎叠加在较低的频率变化,我们平均在6分钟的时间间隔运行和使用平滑数据来推断参数h (t)和z0 (t),叶受到的压力平衡磁场B (t)。在先前的研究中,使用的空间梯度现在提供的集群磁力计被不可用或不在早期研究中受到限制。计算half-thicknesses磁性层的上下文通过检查厚度的变化亚暴阶段三个案例研究事件和21事件的叠加分析时代。在许多情况下,推断half-thickness经历反映了名义上的变化等离子体片在亚暴的(也就是,变薄在成长阶段,增厚亚暴发作)。的相对贡献? B Z / ?在亚暴的cross-tail电流密度。发现B Z / ?部分cross-tail当前亚暴发病。

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