论文标题
三维太阳活性区磁液静态模型及其使用Euler电位的稳定性
Three-dimensional solar active region magnetohydrostatic models and their stability using Euler potentials
论文作者
论文摘要
活动区域(ARS)是在太阳大气中发现的典型磁性结构。我们计算了几种磁液静态(MHS)平衡模型,其中包括有限等离子体$β$和重力的效果,并且在三个维度上代表了这些结构。模型的构建基于使用两个Euler电位,即$α$和$β$,它们代表磁场为$ {\ bf b} = \nablaα\ times \ times \ nablaβ$。理想的MHS非线性偏微分方程是使用固定3D矩形域中的有限元来求解的。最初选择边界条件对应于具有相应Euler电位的已知分析表达式的潜在磁场(无电流)。独特的特征是,我们通过逐渐变形初始电势磁场来结合剪切的效果。此过程非常通用,使我们能够生成各种MHS模型。 AR的热结构通过气压和温度对Euler电位的依赖性结合。使用这种方法,我们实现了ARS中发现的特征热等离子体,但我们证明该方法也可以应用于使用开放磁场线的研究配置。此外,我们研究了包括中性线的基本拓扑。我们的重点是结构的力平衡,我们不考虑构造模型中的能量平衡。此外,我们解决了计算出的3D模型稳定性的困难问题。我们发现,如果等离子体对流稳定,那么系统通常不容易发展磁性雷利 - 泰勒的不稳定性。
Active regions (ARs) are typical magnetic structures found in the solar atmosphere. We calculate several magnetohydrostatic (MHS) equilibrium models that include the effect of a finite plasma-$β$ and gravity and that are representative of these structures in three dimensions. The construction of the models is based on the use of two Euler potentials, $α$ and $β$, that represent the magnetic field as ${\bf B}=\nabla α\times \nabla β$. The ideal MHS nonlinear partial differential equations are solved numerically using finite elements in a fixed 3D rectangular domain. The boundary conditions are initially chosen to correspond to a potential magnetic field (current-free) with known analytical expressions for the corresponding Euler potentials. The distinctive feature is that we incorporate the effect of shear by progressively deforming the initial potential magnetic field. This procedure is quite generic and allows us to generate a vast variety of MHS models. The thermal structure of the ARs is incorporated through the dependence of gas pressure and temperature on the Euler potentials. Using this method we achieve the characteristic hot and over-dense plasma found in ARs, but we demonstrate that the method can also be applied to study configurations with open magnetic field lines. Furthermore, we investigate basic topologies that include neutral lines. Our focus is on the force balance of the structures and we do not consider the energy balance in the constructed models. In addition, we address the difficult question of the stability of the calculated 3D models. We find that if the plasma is convectively stable, then the system is not prone in general to develop magnetic Rayleigh-Taylor instabilities.