Open AccessThe tidal stripping of satellites
Author(s) -
Read J. I.,
Wilkinson M. I.,
Evans N. W.,
Gilmore G.,
Kleyna Jan T.
Publication year - 2006
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2005.09861.x
Subject(s) - physics , radius , orbit (dynamics) , astrophysics , circular orbit , satellite , satellite galaxy , galaxy , astronomy , dwarf galaxy , computer security , computer science , engineering , aerospace engineering
We present an improved analytic calculation for the tidal radius of satellites and test our results against N ‐body simulations. The tidal radius in general depends upon four factors: the potential of the host galaxy, the potential of the satellite, the orbit of the satellite and the orbit of the star within the satellite . We demonstrate that this last point is critical and suggest using three tidal radii to cover the range of orbits of stars within the satellite. In this way we show explicitly that prograde star orbits will be more easily stripped than radial orbits; while radial orbits are more easily stripped than retrograde ones. This result has previously been established by several authors numerically, but can now be understood analytically. For point mass, power‐law (which includes the isothermal sphere), and a restricted class of split power‐law potentials our solution is fully analytic. For more general potentials, we provide an equation which may be rapidly solved numerically. Over short times (≲1–2 Gyr ∼1 satellite orbit), we find excellent agreement between our analytic and numerical models. Over longer times, star orbits within the satellite are transformed by the tidal field of the host galaxy. In a Hubble time, this causes a convergence of the three limiting tidal radii towards the prograde stripping radius. Beyond the prograde stripping radius, the velocity dispersion will be tangentially anisotropic.