Comparing AMR and SPH Cosmological Simulations: I. Dark Matter & Adiabatic Simulations
نویسندگان
چکیده
We compare two cosmological hydrodynamic simulation codes in the context of hierarchical galaxy formation: the smoothed particle hydrodynamics (SPH) code ‘GADGET’, and the Eulerian adaptive mesh refinement (AMR) code ‘ENZO’. Both codes represent dark matter with the N-body method, but use different gravity solvers, and fundamentally different approaches for baryonic hydrodynamics. In the Lagrangian SPH-method of GADGET, a recently developed ‘entropy conserving’ formulation of SPH is used, while for the mesh-based ENZO, two different formulations of Eulerian hydrodynamics are employed: the piecewise parabolic method (PPM) and the artificial viscosity-based scheme used in the magnetohydrodynamics code ZEUS. In this paper, we focus on a comparison of cosmological simulations that follow either only dark matter, or also a non-radiative (‘adiabatic’) hydrodynamic gaseous component. We perform multiple simulations using both codes with varying spatial and mass resolution with identical initial conditions. The dark matter-only runs agree generally quite well, provided ENZO is run with a comparatively fine root grid and a low overdensity threshold for mesh refinement, otherwise the abundance of low-mass halos is suppressed. This can be readily understood as a consequence of the hierarchical particle-mesh algorithm used by ENZO to compute gravitational forces, which tends to deliver lower force resolution than the tree-algorithm of GADGET. At comparable force resolution, we find that the latter offers substantially better performance and lower memory consumption than the present gravity solver in ENZO. In simulations that include adiabatic gas dynamics, we find general agreement in the distribution functions of temperature, entropy, and density for gas of moderate to high overdensity, as found inside dark matter halos. However, there are also some significant differences in the same quantities for gas of lower overdensity. For example, at z = 3, the fraction of cosmic gas that has temperature logT > 0.5 is ∼ 80% for both ENZO/ZEUS and GADGET, while it is 40−60% for ENZO/PPM. We argue that these discrepancies are presumably owing to differences in the shock-capturing abilities of the different methods. In particular, we find that the ZEUS implementation of artificial viscosity in ENZO leads to some unphysical heating at early times in preshock regions. While this is apparently a much weaker effect in GADGET, its use of an artificial viscosity technique may also make it prone to some excess generation of entropy which should be absent in ENZO/PPM. Overall, the hydrodynamical results for GADGET are bracketed by those for ENZO/ZEUS and ENZO/PPM, but are closer to ENZO/ZEUS. Subject headings: galaxies: formation — cosmology: theory — methods: numerical Center for Astrophysics and Space Sciences, University of California at San Diego, La Jolla, CA 92093, U.S.A. Email: bwoshea, [email protected] Harvard-Smithsonian Center for Astrophysics 60 Garden St., Cambridge, MA 02138, U.S.A. Email: knagamin, [email protected] Max-Planck-Institut für Astrophysik Karl-Schwarzschild-Straße 1, 85740 Garching bei München,
منابع مشابه
Study of Galaxy Cluster Properties from High-resolution Sph Simulations
We present some of the results of an ongoing collaboration to sudy the dynamical properties of galaxy clusters by means of high resolution adiabatic SPH cosmological simulations. Results from our numerical clusters have been tested against analytical models often used in X-ray observations: β model (isothermal and polytropic) and those based on universal dark matter profiles. We find a universa...
متن کاملCosmological Simulations with Scale-Free Initial Conditions I: Adiabatic Hydrodynamics
We analyze hierarchical structure formation based on scale-free initial conditions in an Einstein-de Sitter universe, including a baryonic component with Ωbary = 0.05. We present three independent, smoothed particle hydrodynamics (SPH) simulations, performed at two resolutions (323 and 643 dark matter and baryonic particles), and with two different SPH codes (TreeSPH and P3MSPH). Each simulatio...
متن کاملOn the " Initial " Angular Momentum of Galaxies
Spherical density profiles and specific angular momentum profiles of Dark Matter halos found in cosmological N–body simulations have been measured extensively. The distribution of the total angular momentum of dark matter halos is also used routinely in semi–analytic modeling of the formation of disk galaxies. However, it is unclear whether the initial (i.e. at the time the halo is assembled) a...
متن کاملOn the Origin of Cores in Simulated Galaxy Clusters
The diffuse plasma that fills galaxy groups and clusters (the intracluster medium, hereafter ICM) is a by-product of galaxy formation. The present thermal state of this gas results from a competition between gas cooling and heating. The heating comes from two distinct sources: gravitational heating associated with the collapse of the dark matter halo and additional thermal input from the format...
متن کاملResponse of Dark Matter Halos to Condensation of Baryons: Cosmological Simulations and Improved Adiabatic Contraction Model
The cooling of gas in the centers of dark matter halos is expected to lead to a more concentrated dark matter distribution. The response of dark matter to the condensation of baryons is usually calculated using the model of adiabatic contraction, which assumes spherical symmetry and circular orbits. In contrast, halos in the hierarchical structure formation scenarios grow via multiple violent m...
متن کامل