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arXiv 0909.2469astro-ph.IMastro-ph.GA
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光滑粒子磁流体力学IV -使用矢量势

Smoothed Particle Magnetohydrodynamics IV - Using the Vector Potential

Daniel J. Price

摘要:

本文研究了利用光滑粒子流体动力学(SPH)方法数值求解磁流体动力学(MHD)方程时,使用矢势作为维持发散约束的手段。我们推导出一个自洽的制定的运动方程,使用变分原理,是由两个感应方程和用于获得的磁场,保证准确和同时守恒的动量,能量和熵的数值方案的旋度算子的数值公式的约束。这导致了一种新的MHD力项的配方,独特的矢量势,这不同于以前的配方。我们还演示了如何耗散项可以正确地制定的矢量势,使熵的贡献是正定的和总能量守恒。在一个标准套件的数值试验在一个,两个和三个维度,我们首先发现,一致的制定的矢量势方程是不稳定的著名的SPH拉伸不稳定性,甚至比在标准的光滑粒子磁流体力学(SPMHD)制定的磁场是直接演变。此外,我们发现,虽然一个混合的方法的基础上的矢量势演化方程加上一个标准的力项给出了良好的结果为一个和两个维度的问题(其中dAz/dt = 0),这样的方法遭受数值不稳定性在三维相关的矢量势分量的无约束演化。我们的结论是,使用矢量势是不是一个可行的方法光滑粒子磁流体动力学。

英文摘要:

In this paper we investigate the use of the vector potential as a means of maintaining the divergence constraint in the numerical solution of the equations of Magnetohydrodynamics (MHD) using the Smoothed Particle Hydrodynamics (SPH) method. We derive a self-consistent formulation of the equations of motion using a variational principle that is constrained by the numerical formulation of both the induction equation and the curl operator used to obtain the magnetic field, which guarantees exact and simultaneous conservation of momentum, energy and entropy in the numerical scheme. This leads to a novel formulation of the MHD force term, unique to the vector potential, which differs from previous formulations. We also demonstrate how dissipative terms can be correctly formulated for the vector potential such that the contribution to the entropy is positive definite and the total energy is conserved. On a standard suite of numerical tests in one, two and three dimensions we find firstly that the consistent formulation of the vector potential equations is unstable to the well-known SPH tensile instability, even more so than in the standard Smoothed Particle Magnetohydrodynamics (SPMHD) formulation where the magnetic field is evolved directly. Furthermore we find that, whilst a hybrid approach based on the vector potential evolution equation coupled with a standard force term gives good results for one and two dimensional problems (where dAz/dt = 0), such an approach suffers from numerical instability in three dimensions related to the unconstrained evolution of vector potential components. We conclude that use of the vector potential is not a viable approach for Smoothed Particle Magnetohydrodynamics.

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