• DOI:10.1134/1.1575851
• Corpus ID: 11376809

Minimum velocity dispersion in stable stellar disks. Numerical simulations

@article{Khoperskov2003MinimumVD,
  title={Minimum velocity dispersion in stable stellar disks. Numerical simulations},
  author={Alexander V. Khoperskov and Anatolii Vladimirovich Zasov and N. V. Tyurina},
  journal={Astronomy Reports},
  year={2003},
  volume={47},
  pages={357-376}
}

• A. Khoperskov, A. Zasov, N. Tyurina
• Published 10 June 2003
• Physics, Geology
• Astronomy Reports

N-body dynamical simulations are used to analyze the conditions for the gravitational stability of a three-dimensional stellar disk in the gravitational field of two rigid spherical components—a bulge and halo whose central concentrations and relative masses vary over wide ranges. The number of point masses N in the simulations varies from 40 to 500 000 and the evolution of the simulated systems is followed over 10–20 rotation periods of the outer edge of the disk. The initially unstable disks are heated and, as a rule, reach a quasi-stationary equilibrium with a steady-state radial-velocity dispersion cr over five to eight turns. The radial behavior of the Toomre stability parameter QT(r) for the final state of the disk is estimated. Simple models are used to analyze the dependence of the gravitational stability of the disk on the relative masses of the spherical components, disk thickness, degree of differential rotation, and initial state of the disk. Formal application of existing, analytical, local criteria for marginal stability of the disk can lead to errors in cr of more than a factor of 1.5. It is suggested that the approximate constancy of QT⋍1.2–1.5 for r⋍(1–2)×L (where L is the radial scale of disk surface density), valid for a wide range of models, can be used to estimate upper limits for the mass and density of a disk based on the observed distributions of the rotational velocity of the gaseous component and of the stellar velocity dispersion.