An improved dynamical Poisson equation solver for self-gravity

被引:1
|
作者
Maeda, Ryunosuke [1 ]
Inoue, Tsuyoshi [2 ]
Inutsuka, Shu-ichiro [3 ]
机构
[1] Tohoku Univ, Astron Inst, 6-3 Aramaki,Aoba Ku, Sendai 9808578, Japan
[2] Konan Univ, Dept Phys, Okamoto 8-9-1, Kobe 6588501, Japan
[3] Nagoya Univ, Grad Sch Sci, Dept Phys, Furo Cho,Chikusa Ku, Nagoya 4648602, Japan
关键词
methods:; numerical; ADAPTIVE MESH REFINEMENT;
D O I
10.1093/mnras/stad3147
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Since self-gravity is crucial in the structure formation of the Universe, many hydrodynamics simulations with the effect of self-gravity have been conducted. The multigrid method is widely used as a solver for the Poisson equation of the self-gravity; however, the parallelization efficiency of the multigrid method becomes worse when we use a massively parallel computer, and it becomes inefficient with more than 10(4) cores, even for highly tuned codes. To perform large-scale parallel simulations (>10(4) cores), developing a new gravity solver with good parallelization efficiency is beneficial. In this article, we develop a new self-gravity solver using the telegraph equation with a damping coefficient, kappa. Parallelization is much easier than the case of the elliptic Poisson equation since the telegraph equation is a hyperbolic partial differential equation. We analyse convergence tests of our telegraph equations solver and determine that the best non-dimensional damping coefficient of the telegraph equations is kappa similar or equal to 2.5. We also show that our method can maintain high parallelization efficiency even for massively parallel computations due to the hyperbolic nature of the telegraphic equation by weak-scaling tests. If the time-step of the calculation is determined by heating/cooling or chemical reactions, rather than the Courant-Friedrichs-Lewy (CFL) condition, our method may provide the method for calculating self-gravity faster than other previously known methods such as the fast Fourier transform and multigrid iteration solvers because gravitational phase velocity determined by the CFL condition using these time-scales is much larger than the fluid velocity plus sound speed.
引用
收藏
页码:471 / 477
页数:7
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