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首页> 外文期刊>Astrophysics and Space Science >Multicomponent theory of buoyancy instabilities in magnetized plasmas: the case of magnetic field parallel to gravity
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Multicomponent theory of buoyancy instabilities in magnetized plasmas: the case of magnetic field parallel to gravity

机译:磁化等离子体中浮力不稳定性的多成分理论:平行于重力的磁场

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We investigate electromagnetic buoyancy instabilities of the electron-ion plasma with the heat flux based on not the magnetohydrodynamic (MHD) equations, but using the multicomponent plasma approach when the momentum equations are solved for each species. We consider a geometry in which the background magnetic field, gravity, and stratification are directed along one axis. The nonzero background electron thermal flux is taken into account. Collisions between electrons and ions are included in the momentum equations. No simplifications usual for the one-fluid MHD-approach in studying these instabilities are used. We derive a simple dispersion relation, which shows that the thermal flux perturbation generally stabilizes an instability for the geometry under consideration. This result contradicts to conclusion obtained in the MHD-approach. We show that the reason of this contradiction is the simplified assumptions used in the MHD analysis of buoyancy instabilities and the role of the longitudinal electric field perturbation which is not captured by the ideal MHD equations. Our dispersion relation also shows that the medium with the electron thermal flux can be unstable, if the temperature gradients of ions and electrons have the opposite signs. The results obtained can be applied to the weakly collisional magnetized plasma objects in laboratory and astrophysics.
机译:我们不是根据磁流体动力学(MHD)方程而是使用多组分等离子体方法研究每种物质的动量方程时,研究具有热通量的电子离子等离子体的电磁浮力不稳定性。我们考虑一种几何结构,其中背景磁场,重力和分层沿一个轴定向。考虑了非零背景电子热通量。电子和离子之间的碰撞包括在动量方程中。没有使用通常的简化方法来研究这些不稳定性的单流体MHD方法。我们得出一个简单的色散关系,该关系表明热通量扰动通常会稳定所考虑几何形状的不稳定性。该结果与MHD方法中得出的结论相矛盾。我们表明,这一矛盾的原因是在MHD浮力不稳定性分析中使用的简化假设以及理想MHD方程无法捕获的纵向电场扰动的作用。我们的色散关系还表明,如果离子和电子的温度梯度具有相反的符号,则具有电子热通量的介质可能会不稳定。所得结果可应用于实验室和天体物理学中的弱碰撞磁化等离子体对象。

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