NONLINEAR HYDRODYNAMICS OF COSMOLOGICAL SHEETS .2. FRAGMENTATION AND THE GRAVITATIONAL, COOLING, AND THIN-SHELL INSTABILITIES

Citation
Wy. Anninos et al., NONLINEAR HYDRODYNAMICS OF COSMOLOGICAL SHEETS .2. FRAGMENTATION AND THE GRAVITATIONAL, COOLING, AND THIN-SHELL INSTABILITIES, The Astrophysical journal, 450(1), 1995, pp. 1-13
Citations number
37
Categorie Soggetti
Astronomy & Astrophysics
Journal title
ISSN journal
0004637X
Volume
450
Issue
1
Year of publication
1995
Part
1
Pages
1 - 13
Database
ISI
SICI code
0004-637X(1995)450:1<1:NHOCS.>2.0.ZU;2-E
Abstract
Two-dimensional numerical simulations of cosmological sheets are carri ed out to investigate nonlinear hydrodynamical effects on the formatio n of structures such as protogalaxies in the universe. We follow the m otion of both baryonic and dark matter in a postrecombination Friedman n model universe with Omega(0) = 1, Omega(b) = 0.1, and H-0 = 75 km s( -1) Mpc(-1) at scales (less than or equal to 10 Mpc) much smaller than the horizon size. We use a nonuniformly gridded code, composed of the Eulerian hydrodynamic solver ZEUS-2D modified for cosmology and a two -dimensional particle-mesh algorithm, to provide adequate resolution t hroughout the sheet structures. Our simulations allow us to examine in detail the role that nonlinear gravitational, cooling, and thin-shell instabilities play in the fragmentation of cosmological sheets. We co mpute characteristic fragmentation time and length scales for a variet y of initial data and symmetries across the midplane. We find that alt hough the fragmentation time is dependent on the power in the fluctuat ion spectrum, the average size of the protogalactic objects which form by the end of the fragmentation process (z greater than or similar to 2.4) is similar in all cases studied, ranging from 8 to 13 kpc in the plane of collapse with masses of the order of a few times 10(8) M. fo r both the baryonic and the dark matter. We also find that in relaxing reflection symmetry across the midplane, a thin-shell instability act s as early times to excite the bending modes of the cold layer at scal es set by kL similar to 0.1, where k is the transverse wavenumber and L is the pancake thickness, significantly increasing the turbulence an d local vorticity of the pancake.