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arXiv 2102.09952astro-ph.SR
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太阳大气中三角形喷流的扭结不稳定性

Kink instability of triangular jets in the solar atmosphere

T. V. Zaqarashvili, S. Lomineishvili, P. Leitner, A. Hanslmeier, P. Gömöry, M. Roth

摘要:

三角形射流在反对称扭折扰动下是不稳定的。加入磁场可以使射流稳定。喷流和复杂的磁场在太阳大气中普遍存在,这表明在某些情况下存在扭结不稳定性的可能性。本文的目的是研究夹在磁性管/板之间的三角形喷流的扭结不稳定性及其与太阳大气中喷流观测特性的可能联系。通过对射流边界解析解的匹配,得到了控制扭结扰动的色散方程。对不同的射流参数和周围等离子体参数,用解析法和数值法求解了该方程。解析解是伴随着一个完全非线性MHD方程的数值模拟的太阳II型针状体的特定情况。MHD三角形射流的不稳定性取决于Alfven马赫数(流量与Alfven速度之比)和内外密度比。当喷流与周围的等离子体具有相同的密度时,只有超阿尔文流是不稳定的。然而,更密集的射流是不稳定的亚Alfvenic制度。与周围磁场成一定角度的射流比场向流动的不稳定性阈值低得多。扭结不稳定性的增长时间估计为6-15分钟的I型针状体和5-60秒的II型针状体匹配其观察到的寿命。全非线性方程的数值模拟表明,横向扭折脉冲局部破坏射流在不到一分钟的条件下的II型针状。动态扭折不稳定性可能会导致MHD流的完全崩溃,从而观察到太阳大气中针状体的消失。

英文摘要:

It is known that hydrodynamic triangular jets are unstable to antisymmetric kink perturbations. The inclusion of magnetic field may lead to the stabilisation of the jets. Jets and complex magnetic fields are ubiquitous in the solar atmosphere, which suggests the possibility of the kink instability in certain cases. The aim of the paper is to study the kink instability of triangular jets sandwiched between magnetic tubes/slabs and its possible connection to observed properties of the jets in the solar atmosphere. A dispersion equation governing the kink perturbations is obtained through matching of analytical solutions at the jet boundaries. The equation is solved analytically and numerically for different parameters of jets and surrounding plasma. The analytical solution is accompanied by a numerical simulation of fully nonlinear MHD equations for a particular situation of solar type II spicules. MHD triangular jets are unstable to the dynamic kink instability depending on the Alfven Mach number (the ratio of flow to Alfven speeds) and the ratio of internal and external densities. When the jet has the same density as the surrounding plasma, then only super Alfvenic flows are unstable. However, denser jets are unstable also in sub Alfvenic regime. Jets with an angle to the ambient magnetic field have much lower thresholds of instability than field-aligned flows. Growth times of the kink instability are estimated as 6-15 min for type I spicules and 5-60 s for type II spicules matching with their observed life times. Numerical simulation of full nonlinear equations shows that the transverse kink pulse locally destroys the jet in less than a minute in the conditions of type II spicules. Dynamic kink instability may lead to full breakdown of MHD flows and consequently to observed disappearance of spicules in the solar atmosphere.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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