Dynamical friction in constant density cores: a failure of the Chandrasekhar formula
arXiv:astro-ph/0606636 · doi:10.1111/j.1365-2966.2006.11022.x
Abstract
Using analytic calculations and N-body simulations we show that in constant density (harmonic) cores, sinking satellites undergo an initial phase of very rapid (super-Chandrasekhar) dynamical friction, after which they experience no dynamical friction at all. For density profiles with a central power law profile of log-slope, , the infalling satellite heats the background and causes to decrease. For initially, the satellite generates a small central constant density core and stalls as in the case. We discuss some astrophysical applications of our results to decaying satellite orbits, galactic bars and mergers of supermassive black hole binaries. In a companion paper we show that a central constant density core can provide a natural solution to the timing problem for Fornax's globular clusters.
11 pages, 7 figures. Final version accepted for publication in MNRAS
References in corpus (2)
Cited by in corpus (10)
- The ACS Virgo Cluster Survey. XII. The Luminosity Function of Globular Clusters in Early Type Galaxies
- Ejection of Supermassive Black Holes from Galaxy Cores
- The nucleus of the Sagittarius dSph galaxy and M54: a window on the process of galaxy nucleation
- The Causes of Halo Shape Changes Induced by Cooling Baryons: Disks Versus Substructures
- Small Dwarf Galaxies Within Larger Dwarfs: Why Some Are Luminous While Most Go Dark
- The formation of ultra-compact dwarf galaxies and nucleated dwarf galaxies
- Self-consistent simulations of Nuclear Cluster formation through Globular Cluster orbital decay and merging
- Dynamical friction of massive objects in galactic centres
- Constraints on the merging timescale of luminous red galaxies, or, where do all the halos go?
- Constraining dark matter sub-structure with the dynamics of astrophysical systems