Abstract
We describe the interplay between stellar evolution and dynamical mass loss of evolving star
clusters, based on the principles of stellar evolution and cluster dynamics and on the details
of a grid of N-body simulations of Galactic cluster models. The cluster models have different
initial masses, different orbits, including elliptical ones, and different initial density profiles.
We use two sets of cluster models: one set of Roche lobe filling models and a new set of cluster
models that are initially underfilling their tidal radius.
We identify four distinct mass-loss effects: (1) mass loss by stellar evolution, (2) loss of
stars induced by stellar evolution and (3) relaxation-driven mass loss before and (4) after
core collapse. At young ages the mass loss is dominated by stellar evolution, followed by the
evolution-induced loss of stars. This evolution-induced mass loss is important if a cluster is
immersed in the tidal field. Both the evolution-induced loss of stars and the relaxation-driven
mass loss need time to build up. This is described by a delay function that has a characteristic
time-scale of a few crossing times for Roche lobe filling clusters and a few half-mass relaxation
times for initially Roche lobe underfilling clusters. The relaxation-driven mass loss (called
‘dissolution’ in this paper) can be described by a simple power-law dependence of the mass
d(M/M )/dt = −(M/M )1−γ /t0, where t0 depends on the orbit and environment of the
cluster. The index γ is 0.65 for clusters with a King parameter W0 = 5 for the initial density
distribution, and 0.80 for more concentrated clusters with W0 = 7. For initially Roche lobe
underfilling clusters the dissolution is described by the same γ =0.80, independent of the initial
density distribution. The values of the constant t0 are derived for the models and described
by simple formulae that depend on the orbit of the cluster. The mass-loss rate increases by
about a factor of 2 at core collapse and the mass dependence of the relaxation-driven mass
loss changes to γ = 0.70 after core collapse.
We also present a simple recipe for predicting the mass evolution of individual star clusters
with various metallicities and in different environments, with an accuracy of a few per cent in
most cases. This can be used to predict the mass evolution of cluster systems.
Original language | English |
---|---|
Pages (from-to) | 305-328 |
Number of pages | 24 |
Journal | Monthly Notices of the Royal Astronomical Society |
Volume | 409 |
Issue number | 1 |
DOIs | |
Publication status | Published - 2010 |