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arXiv 1303.4130astro-ph.SR
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日冕通量管倾角对日珥物质的支持

On the Support of Solar Prominence Material by the Dips of a Coronal Flux Tube

Andrew Hillier, Adriaan van Ballegooijen

摘要:

致密的日珥物质被认为是通过下沉日冕磁场的磁张力来抵抗重力的。对于静态磁场,它表现出许多重力驱动的流动,水动力可能会发挥重要作用,在确定的大规模和小规模的磁场分布。在这项研究中,我们提出了第一个步骤,建立三维磁流体静力学日珥模型,其中日珥是在一个日冕通量管的倾角形成。在这里,2.5D平衡是通过将质量添加到最初的无力磁场,然后执行二次磁流体动力学弛豫来创建的。详细研究了两种相反极性的磁场配置,一个简单的o点配置的水平场(B_x)与轴向场(B_y)的比例为1:2和一个更复杂的模型,也有一个x点的比例为1:11。该模型表明,对重力的支持是由总压力或张力,只有张力支持类似于观察到的静态阻力。日冕通量管的o点被日珥物质拉下,导致日珥底部的磁场压缩。因此,张力支撑来自于底部压缩磁场的小曲率和日珥顶部拉伸磁场的大曲率。结果发现,这种方法并不能保证收敛到一个类似于连续平衡的情况下,存在一个x点的日珥通量管。结果表明,等离子体β值约为0.1是必要的,以支持通过磁张力的双折射。

英文摘要:

The dense prominence material is believed to be supported against gravity through the magnetic tension of dipped coronal magnetic field. For quiescent prominences, which exhibit many gravity-driven flows, hydrodynamic forces are likely to play an important role in the determination of both the large and small scale magnetic field distributions. In this study, we present the first steps toward creating three-dimensional magneto-hydrostatic prominence model where the prominence is formed in the dips of a coronal flux tube. Here 2.5D equilibria are created by adding mass to an initially force-free magnetic field, then performing a secondary magnetohydrodynamic relaxation. Two inverse polarity magnetic field configurations are studied in detail, a simple o-point configuration with a ratio of the horizontal field (B_x) to the axial field (B_y) of 1:2 and a more complex model that also has an x-point with a ratio of 1:11. The models show that support against gravity is either by total pressure or tension, with only tension support resembling observed quiescent prominences. The o-point of the coronal flux tube was pulled down by the prominence material, leading to compression of the magnetic field at the base of the prominence. Therefore tension support comes from the small curvature of the compressed magnetic field at the bottom and the larger curvature of the stretched magnetic field at the top of the prominence. It was found that this method does not guarantee convergence to a prominence-like equilibrium in the case where an x-point exists below the prominence flux tube. The results imply that a plasma beta of ~ 0.1 is necessary to support prominences through magnetic tension.

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