使用矢量势方法的保形运动自适应网格上的无发散磁流体动力学

P. Chris Fragile , Daniel Nemergut , Payden L. Shaw , Peter Anninos
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引用次数: 6

摘要

我们提出了一种新的方法来发展磁流体动力学方程(牛顿和相对论),该方法能够在自适应精细、共形移动的网格上保持无发散磁场(Ş∙B=0)。该方法依赖于演化磁矢量势,然后使用它来重建磁场。这种方法的优点是,矢量势不像磁场那样受到约束方程的约束,因此可以以简单的方式进行细化和移动。我们针对一系列问题测试了这种新方法,从均匀网格上的简单Alfvén波到嵌套球形极网格上黑洞吸积的一般相对论MHD模拟。我们发现,该代码产生了准确的结果,并且在所有情况下都保持了机器精度的无发散磁场。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Divergence-free magnetohydrodynamics on conformally moving, adaptive meshes using a vector potential method

We present a new method for evolving the equations of magnetohydrodynamics (both Newtonian and relativistic) that is capable of maintaining a divergence-free magnetic field (B=0) on adaptively refined, conformally moving meshes. The method relies on evolving the magnetic vector potential and then using it to reconstruct the magnetic fields. The advantage of this approach is that the vector potential is not subject to a constraint equation in the same way the magnetic field is, and so can be refined and moved in a straightforward way. We test this new method against a wide array of problems from simple Alfvén waves on a uniform grid to general relativistic MHD simulations of black hole accretion on a nested, spherical-polar grid. We find that the code produces accurate results and in all cases maintains a divergence-free magnetic field to machine precision.

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来源期刊
Journal of Computational Physics: X
Journal of Computational Physics: X Physics and Astronomy-Physics and Astronomy (miscellaneous)
CiteScore
6.10
自引率
0.00%
发文量
7
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