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Large-scale zonal structures and short scale spectra generated by drift flute waves in high-beta hed plasmas

机译:在高β铰接等离子体中漂移长笛波产生的大规模区间结构和短尺度光谱

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Our aim is to develop a more general analysis of nonlinear dynamics of drift-flute waves, applicable to arbitrary plasma beta and arbitrary spatial scales in comparison with the ion Larmor radius. This study is of interest for fundamental plasma theory as well as for the interpretation of Z-pinch and laboratory astrophysics experiments. Description of low-frequency waves and in particular drift flute waves in a high beta plasma, generally speaking, requires a kinetic approach, based on the Vlasov- Maxwell set of equations. In the present work we show that the alternative two-fluid approach can adequately describe the ion perturbations with arbitrary ratio of the characteristic spatial scales to the ion Larmor radius in so-called Pade approximation. For this purpose reduced two-fluid hydrodynamic equations which describe nonlinear dynamics of the flute waves with arbitrary spatial scales and arbitrary plasma beta are derived. The linear dispersion relation of the flute waves and the Rayleigh-Taylor instability are analyzed. A general nonlinear dispersion relation which describes generation of large-scale zonal structures by the flute waves is presented and analyzed.
机译:我们的目的是开发更一般性地分析漂移槽波的非线性动力学,适用于与离子拉马尔半径相比的任意等离子体β和任意空间尺度。本研究对基本等离子体理论来说感兴趣,以及解释Z-Pinch和实验室天体物理实验。低频波和特定的漂移长笛波在高β等离子体中,一般而言,需要一种动力学方法,基于方程式的Vlasov-Maxwell集。在本工作中,我们表明,替代的双流体方法可以充分描述具有特征空间尺度的任意比率的离子扰动,以便在所谓的梯队近似下的离子传道半径。为此目的,减少了描述具有任意空间尺度的长笛波的非线性动力学和任意等离子体β的双流体流体动力学等式。分析了长笛波和瑞利 - 泰勒不稳定性的线性分散关系。提出并分析了描述由长笛波产生大规模区间结构产生的一般非线性分散关系。

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