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arXiv 0709.3687astro-phphysics.plasm-phphysics.space-ph
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日冕加热Parker情景的非线性动力学

Nonlinear Dynamics of the Parker Scenario for Coronal Heating

A. F. Rappazzo, M. Velli, G. Einaudi, R. B. Dahlburg

摘要:

通过在约化磁流体力学(RMHD)框架内对日冕环在日冕几何中的动力学进行长时间高分辨率模拟,全面研究了日冕加热的Parker或磁力线缠结模型。缓慢的光球运动诱导坡印廷通量饱和驱动的各向异性湍流级联占主导地位的磁能。在物理空间中,这对应于磁拓扑,其中磁场线几乎没有纠缠,然而电流片(对应于帕克假设的原始切向不连续性)连续地形成和消散。电流片是非线性级联的结果,该级联将能量从对流运动尺度($\sim 1,000 km$)向下转移到耗散尺度,在耗散尺度处,能量最终转换为热量和/或粒子加速。电流片构成了系统的耗散结构,与之相关的磁重联在小尺度上引起脉冲“突发”加热事件。这张照片与最先进的(E)UV和X射线成像仪观察到的细长环是一致的,这些成像仪虽然表面上是静止的,但在这些波长下闪耀着明亮的光芒,几乎没有纠缠特征的证据。弱和强的MHD湍流的发展,以及它们对日冕加热定标的影响,不同的制度,被证明取决于环路参数,这种依赖性的定量特征:弱湍流制度和陡峭的光谱发生在{ \it较强的环路领域},并导致{ \it较大的加热率}比在弱场区域。

英文摘要:

The Parker or field line tangling model of coronal heating is studied comprehensively via long-time high-resolution simulations of the dynamics of a coronal loop in cartesian geometry within the framework of reduced magnetohydrodynamics (RMHD). Slow photospheric motions induce a Poynting flux which saturates by driving an anisotropic turbulent cascade dominated by magnetic energy. In physical space this corresponds to a magnetic topology where magnetic field lines are barely entangled, nevertheless current sheets (corresponding to the original tangential discontinuities hypothesized by Parker) are continuously formed and dissipated. Current sheets are the result of the nonlinear cascade that transfers energy from the scale of convective motions ($\sim 1,000 km$) down to the dissipative scales, where it is finally converted to heat and/or particle acceleration. Current sheets constitute the dissipative structure of the system, and the associated magnetic reconnection gives rise to impulsive ``bursty'' heating events at the small scales. This picture is consistent with the slender loops observed by state-of-the-art (E)UV and X-ray imagers which, although apparently quiescent, shine bright in these wavelengths with little evidence of entangled features. The different regimes of weak and strong MHD turbulence that develop, and their influence on coronal heating scalings, are shown to depend on the loop parameters, and this dependence is quantitatively characterized: weak turbulence regimes and steeper spectra occur in {\it stronger loop fields} and lead to {\it larger heating rates} than in weak field regions.

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