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arXiv 1608.00541math.NAcs.NA
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基于场线积分的强各向异性扩散方程的渐近保留方法

An Asymptotic Preserving method for strongly anisotropic diffusion equations based on field line integration

Institute of natural sciences and department of mathematics, Shanghai Jiao Tong University(上海交通大学自然科学与数学系)

Min Tang, Yihong Wang

AI总结:

本文提出一种基于场线积分的渐近保留方法,用于解决强各向异性扩散方程中的病态问题,通过替换Neumann边界条件以积分形式,消除奇异项,实现问题的良定。

摘要:

在磁化等离子体中,磁场约束粒子沿场线运动。粘性及热传导的各向异性强度可能达到$10^{12}$量级。当边界条件为周期或Neumann时,强扩散会导致极限问题病态。本文引入一种简单但高效的渐近保留改写方法,关键思想是不局部离散Neumann边界条件,而是用场线积分形式替代其中一个Neumann边界条件,积分后奇异的$1/ε$项被替换为$O(1)$项,从而得到良定问题。对原代码只需小修改,无需改变坐标或适应网格。数值上可观察到关于各向异性强度$1/ε$的均匀收敛性,条件数不随各向异性变化。

英文摘要:

In magnetized plasma, the magnetic field confines the particles around the field lines. The anisotropy intensity in the viscosity and heat conduction may reach the order of $10^{12}$. When the boundary conditions are periodic or Neumann, the strong diffusion leads to an ill-posed limiting problem. To remove the ill-conditionedness in the highly anisotropic diffusion equations, we introduce a simple but very efficient asymptotic preserving reformulation in this paper. The key idea is that, instead of discretizing the Neumann boundary conditions locally, we replace one of the Neumann boundary condition by the integration of the original problem along the field line, the singular $1/ε$ terms can be replaced by $O(1)$ terms after the integration, so that yields a well-posed problem. Small modifications to the original code are required and no change of coordinates nor mesh adaptation are needed. Uniform convergence with respect to the anisotropy strength $1/ε$ can be observed numerically and the condition number does not scale with the anisotropy.

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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