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arXiv 2005.14332astro-ph.SR
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基于SUNRISE/IMaX矢量磁图的AR11768磁流体静力学模拟

Magnetohydrostatic modeling of AR11768 based on a SUNRISE/IMaX vector magnetogram

Xiaoshuai Zhu, Thomas Wiegelmann, Sami Solanki

摘要:

上下文高分辨率的磁场测量通常只在太阳光球层中进行。像色球层和日冕这样的高层可以通过向上外推光球层的磁场来模拟。在日冕中,等离子体力可以忽略,洛伦兹力消失。在上层光球层和色球层中,磁性和非磁力是同等重要的。解决这个问题的一种方法是用磁流体静力学(MHS)模型自洽地计算等离子体和磁场。目标。我们的目标是推导出磁场,等离子体的压力和密度的AR 11768通过应用新开发的外推技术的日出/IMaX数据。方法.采用优化方法对MHS进行建模。初始条件由非线性无力场(NLFFF)和重力层结大气组成。结果在非无力层,这是空间上解决了新的代码,洛伦兹力有效地平衡的气体压力梯度力和重力。在强场区,气压和密度都是亏损的,这与观测结果是一致的。然而,在有源区边缘的某些部分也观察到更致密的等离子体。在色球层中,纤维状等离子体结构很好地跟踪磁场。在日出/SuFI 3000 { $Å$ }图像中的亮点通常伴随着等离子体压力和电流浓度。此外,MHS场线与所选色球纤维之间夹角的平均值为$11.8^\circ$,小于由NLFFF模型($15.7^\circ$)和线性MHS模型($20.9^\circ$)计算的结果。这表明,MHS解决方案提供了一个更好的代表性的磁场在色球层。

英文摘要:

Context. High resolution magnetic field measurements are routinely done only in the solar photosphere. Higher layers like the chromosphere and corona can be modeled by extrapolating the photospheric magnetic field upward. In the solar corona, plasma forces can be neglected and the Lorentz force vanishes. This is not the case in the upper photosphere and chromosphere where magnetic and non-magnetic forces are equally important. One way to deal with this problem is to compute the plasma and magnetic field self-consistently with a magnetohydrostatic (MHS) model. Aims. We aim to derive the magnetic field, plasma pressure and density of AR11768 by applying the newly developed extrapolation technique to the SUNRISE/IMaX data. Methods. An optimization method is used for the MHS modeling. The initial conditions consist of a nonlinear force-free field (NLFFF) and a gravity-stratified atmosphere. Results. In the non-force-free layer, which is spatially resolved by the new code, Lorentz forces are effectively balanced by the gas pressure gradient force and the gravity force. The pressure and density are depleted in strong field regions, which is consistent with observations. Denser plasma, however, is also observed at some parts of the active region edges. In the chromosphere, the fibril-like plasma structures trace the magnetic field nicely. Bright points in SUNRISE/SuFI 3000 {$Å$} images are often accompanied by the plasma pressure and electric current concentrations. In addition, the average of angle between MHS field lines and the selected chromospheric fibrils is $11.8^\circ$, which is smaller than those computed from the NLFFF model ($15.7^\circ$) and linear MHS model ($20.9^\circ$). This indicates that the MHS solution provides a better representation of the magnetic field in the chromosphere.

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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