Fundamental differences between SPH and grid methods

被引:528
作者
Agertz, Oscar [1 ]
Moore, Ben
Stadel, Joachim
Potter, Doug
Miniati, Francesco
Read, Justin
Mayer, Lucio
Gawryszczak, Artur
Kravtosov, Andrey
Nordlund, Ake
Pearce, Frazer
Quilis, Vicent
Rudd, Douglas
Springel, Volker
Stone, James
Tasker, Elizabeth
Teyssier, Romain
Wadsley, James
Walder, Rolf
机构
[1] Univ Zurich, Inst Theoret Phys, CH-8057 Zurich, Switzerland
[2] ETH, Inst Astron, Dept Phys, CH-8093 Zurich, Switzerland
[3] Nicholas Copernicus Astron Ctr, PL-00716 Warsaw, Poland
[4] Univ Chicago, Dept Astron & Astrophys, Chicago, IL 60637 USA
[5] Univ Copenhagen, Niels Bohr Inst, DK-2100 Copenhagen, Denmark
[6] Univ Nottingham, Sch Phys & Astron, Nottingham NG7 2RD, England
[7] Univ Valencia, Dept Astron & Astrophys, E-46100 Burjassot, Spain
[8] Max Planck Inst Astrophys, D-85740 Garching, Germany
[9] Princeton Univ, Dept Astrophys Sci, Princeton, NJ 08544 USA
[10] Columbia Univ, Dept Astron, New York, NY 10027 USA
[11] CEA, DSM, DAPNIA SAp, Ctr Etud Saclay,Serv Astron, F-91191 Gif Sur Yvette, France
[12] McMaster Univ, Dept Phys & Astron, Hamilton, ON L88 4M1, Canada
[13] ETH, Inst Astron, CH-8092 Zurich, Switzerland
关键词
hydrodynamics; instabilities; turbulence; methods : numerical; ISM : clouds; galaxies : evolution; galaxies : formation; galaxies : general;
D O I
10.1111/j.1365-2966.2007.12183.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We have carried out a comparison study of hydrodynamical codes by investigating their performance in modelling interacting multiphase fluids. The two commonly used techniques of grid and smoothed particle hydrodynamics (SPH) show striking differences in their ability to model processes that are fundamentally important across many areas of astrophysics. Whilst Eulerian grid based methods are able to resolve and treat important dynamical instabilities, such as Kelvin-Helmholtz or Rayleigh-Taylor, these processes are poorly or not at all resolved by existing SPH techniques. We show that the reason for this is that SPH, at least in its standard implementation, introduces spurious pressure forces on particles in regions where there are steep density gradients. This results in a boundary gap of the size of an SPH smoothing kernel radius over which interactions are severely damped.
引用
收藏
页码:963 / 978
页数:16
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