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首页> 外文期刊>The Astrophysical journal >PLASMA DYNAMICS OF MAGNETIC FLUX INJECTION IN THE SOLAR ATMOSPHERE
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PLASMA DYNAMICS OF MAGNETIC FLUX INJECTION IN THE SOLAR ATMOSPHERE

机译:太阳大气中磁通量注入的等离子体动力学

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A computational analysis of magnetic flux injection from the solar photosphere into the solar chromosphere and corona is presented. The model is one-dimensional and describes the evolution of the plasma and neutrals in the vertical x-direction; the magnetic field is assumed to be unidirectional in the horizontal plane. The initial magnetic field profile is a step function (a magnetic piston): B = B_0 + ΔB for x ≤ x_0 and B = B_0 for x > x_0. The field is then allowed to relax self-consistently for t > 0 and x > x_(x_0): a shock is launched followed by the relaxation of the magnetic piston. Simulation results are presented for different initial positions x_0 of the field jump in the chromosphere. When the piston (ΔB ~ tens of gauss) is very low in the chromosphere, a weak shock is launched that results in upward plasma and neutral velocities V approx= few km s~(-1) in the upper chromosphere and corona; the plasma and neutrals only attain velocities V approx= tens of m s~(-1) in the lower chromosphere. A quasi-steady state follows, and the piston does not relax significantly because the pressure change across the magnetic piston is small. When the piston is initiated in the upper chromosphere, a stronger shock is launched into the corona; plasma and neutral velocities V approx= tens of km s~(-1) are generated. Subsequently, the magnetic field piston relaxes and penetrates the transition layer into the corona; the upward velocities are V approx= hundreds of km s~(-1). At the same time, plasma and neutrals are being swept into the corona.
机译:提出了从太阳光球注入太阳色球和日冕的磁通量的计算分析。该模型是一维的,描述了等离子体和中性粒子在垂直x方向上的演化;假定磁场在水平面中是单向的。初始磁场分布是一个阶跃函数(一个磁性活塞):对于x≤x_0,B = B_0 +ΔB;对于x> x_0,B = B_0。然后允许磁场在t> 0和x> x_(x_0)时自洽地弛豫:先进行冲击,然后使电磁活塞弛豫。给出了色球中场跳变的不同初始位置x_0的仿真结果。当色球中的活塞(ΔB〜数十高斯)非常低时,会发出微弱的冲击,导致上部色球和电晕中的等离子体和中性速度V大约=几千米s〜(-1)。等离子体和中性粒子仅在较低色球层中达到约V s =(m s〜(-1))的速度。随后达到准稳态,并且由于磁性活塞两端的压力变化较小,因此活塞不会显着松弛。当活塞在上层色球中启动时,会向电晕中发出更强烈的冲击。等离子体和中性速度V大约为几十km s〜(-1)。随后,磁场活塞松弛并穿透过渡层进入电晕。向上的速度是V大约=数百km s〜(-1)。同时,等离子体和中性粒子被扫入电晕。

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