2008MNRAS.386..835L


Query : 2008MNRAS.386..835L

2008MNRAS.386..835L - Mon. Not. R. Astron. Soc., 386, 835-858 (2008/May-2)

Self-similar shocks and winds in galaxy clusters.

LOU Y.-Q., JIANG Y.-F. and JIN C.-C.

Abstract (from CDS):

A theoretical model framework of spherical symmetry is presented for a composite astrophysical system of two polytropic fluids coupled together by gravity to explore large-scale shocks and flow dynamics in clusters of galaxies or in globular clusters. The existence of such large-scale shocks in clusters of galaxies as inferred by high-resolution X-ray and radio imaging observations implies large-scale systematic flows that are beyond usual static models for clusters of galaxies. Here, we explore self-similar two-fluid flow solutions with shocks for a hot polytropic gas flow in a cluster of galaxies in the presence of a massive dark matter (DM) flow after the initiation of a gravitational core collapse or a central active galactic nucleus (AGN) activity or a large-scale merging process. In particular, the possibility of DM shocks or sharp jumps of mass density and of velocity dispersion in DM halo is suggested and such DM shocks might be detectable through gravitational lensing effects. To examine various plausible scenarios for clusters of galaxies, we describe three possible classes of shock flows within our model framework for different types of temperature, density and flow speed profiles. Depending upon sensible model parameters and shock locations, the hot intracluster medium (ICM) and DM halo may have various combinations of asymptotic behaviours of outflow, breeze, inflow, contraction or static envelopes at large radii at a given time. We refer to asymptotic outflows of hot ICM at large radii as the galaxy cluster wind. As a result of such galaxy cluster winds and simultaneous contractions of DM halo during the course of galaxy cluster evolution, there would be less hot ICM within clusters of galaxies as compared to the average baryon fraction in the Universe. Physically, it is then expected that such `missing baryons' with lower temperatures reside in the periphery of galaxy clusters on much larger scales. Based on our model analysis, we also predict a limiting (the steepest) radial scaling form for mass density profiles of r–3 within clusters of galaxies.

Abstract Copyright: © 2008 The Authors. Journal compilation © 2008 RAS

Journal keyword(s): gravitation - hydrodynamics - shock waves - galaxies: clusters: general - dark matter - X-rays: galaxies: clusters

Simbad objects: 26

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Number of rows : 26
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 ACO 85 ClG 00 41 36.21 -09 19 30.4           ~ 909 0
2 ACO 262 ClG 01 52 50.4 +36 08 46           ~ 699 1
3 ACO 426 ClG 03 19 47.2 +41 30 47           ~ 2258 1
4 3C 84 Sy2 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4008 3
5 ZwCl 0335+0956 ClG 03 38 35.3 +09 57 54           ~ 383 1
6 ACO 3158 ClG 03 42 39.6 -53 37 50           ~ 304 0
7 ACO 520 ClG 04 54 10.1 +02 55 38           ~ 436 0
8 ACO 3376 ClG 06 01 25.000 -39 59 51.00           ~ 305 0
9 ClG 0657-56 ClG 06 58 29.6 -55 56 39           ~ 963 1
10 ZwCl 0735+7421 ClG 07 41 40.3 +74 14 58     17.70     ~ 254 0
11 ACO 644 ClG 08 17 24.5 -07 30 46           ~ 225 0
12 ACO 665 ClG 08 30 45.2 +65 52 55           ~ 437 0
13 ACO 780 ClG 09 18 30 -12 15.7           ~ 453 0
14 ACO 786 ClG 09 28 04.9 +74 46 58           ~ 43 0
15 NAME Virgo Cluster ClG 12 26 32.1 +12 43 24           ~ 6645 0
16 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2094 2
17 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 4803 2
18 ACO 2052 ClG 15 16 41.64 +07 01 45.5           ~ 730 1
19 ACO 2142 ClG 15 58 14.38 +27 12 57.8           ~ 768 0
20 ACO 2199 ClG 16 28 43.31 +39 34 07.6           ~ 1171 1
21 ACO 2204 ClG 16 32 45.7 +05 34 43           ~ 436 0
22 ACO 2256 ClG 17 03 09.4 +78 39 36           ~ 885 1
23 ACO 2255 ClG 17 12 50.04 +64 03 10.6           ~ 568 0
24 ACO 2319 ClG 19 20 45.3 +43 57 43           ~ 461 1
25 ACO 3667 ClG 20 12 33.68 -56 50 26.3           ~ 627 1
26 ZwCl 2341+0000 ClG 23 43 40.566 +00 18 18.94           ~ 70 0

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