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不可压缩磁流体动力学湍流中各向异性的发展。

Development of anisotropy in incompressible magnetohydrodynamic turbulence.

作者信息

Bigot Barbara, Galtier Sébastien, Politano Hélène

机构信息

Institut d'Astrophysique Spatiale, Bâtiment 121, Université Paris-Sud XI, UMR 8617, 91405 Orsay, France.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Dec;78(6 Pt 2):066301. doi: 10.1103/PhysRevE.78.066301. Epub 2008 Dec 2.

DOI:10.1103/PhysRevE.78.066301
PMID:19256939
Abstract

We present a set of three-dimensional direct numerical simulations of incompressible decaying magnetohydrodynamic turbulence in which we investigate the influence of an external uniform magnetic field B0 . A parametric study in terms of B0 intensity is made where, in particular, we distinguish the shear-from the pseudo-Alfvén waves dynamics. The initial kinetic and magnetic energies are equal with a negligible cross correlation. Both the temporal and spectral effects of B0 are discussed. A subcritical balance is found between the Alfvén and nonlinear times with both a global and a spectral definition. The nonlinear dynamics of strongly magnetized flows is characterized by a different k_{ perpendicular} spectrum (where B0 defines the parallel direction) if it is plotted at a fixed k_{ parallel} (two-dimensional spectrum) or if it is integrated (averaged) over all k_{ parallel} (one-dimensional spectrum). In the former case a much wider inertial range is found with a steep power law, closer to the wave turbulence prediction than the Kolmogorov one such as in the latter case. It is believed that the averaging effect may be a source of difficulty to detect the transition towards wave turbulence in natural plasmas. Another important result of this paper is the formation of filaments reported within current and vorticity sheets in strongly magnetized flows, which modifies our classical picture of dissipative sheets in conductive flows.

摘要

我们给出了一组不可压缩衰减磁流体动力学湍流的三维直接数值模拟,其中我们研究了外部均匀磁场B0的影响。针对B0强度进行了参数研究,特别是区分了剪切波与伪阿尔文波的动力学。初始动能和磁能相等,交叉相关性可忽略不计。讨论了B0的时间和频谱效应。在阿尔文时间和非线性时间之间发现了一种亚临界平衡,既有全局定义也有频谱定义。如果在固定的k平行(二维频谱)下绘制,或者在所有k平行(一维频谱)上积分(平均),强磁化流的非线性动力学由不同的k垂直频谱(其中B0定义平行方向)表征。在前一种情况下,发现了一个更宽的惯性范围,具有陡峭的幂律,比后一种情况更接近波湍流预测,而不是柯尔莫哥洛夫预测。据信,平均效应可能是在自然等离子体中检测向波湍流转变的一个困难来源。本文的另一个重要结果是在强磁化流的电流和涡度片中报告了细丝的形成,这改变了我们对导电流中耗散片的经典认识。

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