K. Saigo et al., Collapse of rotating gas clouds and formation of protostellar disks: Effects of temperature change during collapse, ASTROPHYS J, 531(2), 2000, pp. 971-987
We show two-dimensional numerical simulations of the gravitational collapse
of rotating gas clouds. We assume the polytropic equation of state, P = K
rho(gamma), to take account of the temperature change during the collapse.
Our numerical simulations have two model parameters, beta and gamma, which
specify the initial rotation velocity and polytropic index, respectively. W
e show three models, beta = 1.0, 0.5, and 0.2, for each gamma, which is tak
en to be 0.8, 0.9, 0.95, 1.05, 1.1, or 1.2. These 18 models are compared wi
th previously reported isothermal models (gamma = 1). In each model a rotat
ing cylindrical cloud initially in equilibrium fragments periodically becau
se of the growth of a velocity perturbation and forms cloud cores. The clou
d core becomes a dynamically collapsing gaseous disk whose central density
(rho(c)) increases with time (t) in proportion to rho(c) proportional to (t
- t(0))(-2). This collapse is qualitatively similar in density and velocit
y distributions to the runaway collapse of a rotating isothermal cloud. The
surface density of the disk, Sigma, is proportional to the power of the ra
dial distance, Sigma(r) proportional to r(1-2 gamma), in the envelope. Mode
ls with gamma > 1 have geometrically thick disks (aspect ratio r(d)/z(d) si
milar or equal to 2), while those with gamma < 1 have very thin disks (r(d)
/z(d) > 10). While the former disks are stable, the latter disks are unstab
le against fragmentation if we adopt the Toomre stability criterion for a t
hin gaseous disk. Our numerical simulations also show the growth of a rotat
ionally supported disk by radial accretion in a period t > t(0) for models
with gamma > 1. The accretion phase starts at a stage in which the central
density is still finite. The central density at the beginning of the accret
ion phase is lower when beta and gamma are larger. Our models with gamma >
1 are applicable to star formation in turbulent gas clouds in which the eff
ective sound speed decreases with increase in the density. Our models with
gamma > 1 are applicable to star formation in primordial clouds in which th
e temperature increase during the collapse is due to less efficient cooling
.