Self‐regulated gravitational accretion in protostellar discs

We present a numerical model for the evolution of a protostellar disc that has formed self-consistently from the collapse of a molecular cloud core. The global evolution of the disc is followed for several million years after its formation. The capture of a wide range of spatial and temporal scales is made possible by use of the thin-disc approximation. We focus on the role of gravitational torques in transporting mass inward and angular momentum outward during different evolutionary phases of a protostellar disc with disc-to-star mass ratio of order 0.1. In the early phase, when the infall of matter from the surrounding envelope is substantial, mass is transported inward by the gravitational torques from spiral arms that are a manifestation of the envelope-induced gravitational instability in the disc. In the late phase, when the gas reservoir of the envelope is depleted, the distinct spiral structure is replaced by ongoing irregular non-axisymmetric density perturbations. The amplitude of these density perturbations decreases with time, though this process is moderated by swing amplification aided by the existence of the disc's sharp outer edge. Our global modelling of the protostellar disc reveals that there is typically a residual non-zero gravitational torque from these density perturbations, i.e. their effects do not exactly cancel out in each region. In particular, the net gravitational torque in the inner disc tends to be negative during first several million years of the evolution, while the outer disc has a net positive gravitational torque. Our global model of a self-consistently formed disc shows that it is also self-regulated in the late phase, so that it is near the Toomre stability limit, with a near-uniform Toomre parameter Q ≈ 1.5-2.0. Since the disc also has near-Keplerian rotation, and comparatively weak temperature variation, it maintains a near-power-law surface density profile proportional to r -3/2 .

[1]  Cambridge,et al.  Testing the locality of transport in self-gravitating accretion discs — II. The massive disc case , 2005 .

[2]  The effect of a finite mass reservoir on the collapse of spherical isothermal clouds and the evolution of protostellar accretion , 2005, astro-ph/0504055.

[3]  J. Hawley,et al.  Instability, turbulence, and enhanced transport in accretion disks , 1997 .

[4]  R. Larson Gravitational torques and star formation , 1984 .

[5]  The Effect of Internal Dissipation and Surface Irradiation on the Structure of Disks and the Location of the Snow Line around Sun-like Stars , 2006, astro-ph/0605110.

[6]  Boltzmann moment equation approach for the numerical study of anisotropic stellar discs , 2006, astro-ph/0609250.

[7]  P. Goldreich,et al.  Spectral Energy Distributions of T Tauri Stars with Passive Circumstellar Disks , 1997, astro-ph/9706042.

[8]  S. Basu A Semianalytic Model for Supercritical Core Collapse: Self-Similar Evolution and the Approach to Protostar Formation , 1997 .

[9]  Charles F. Gammie,et al.  Layered Accretion in T Tauri Disks , 1996 .

[10]  Cambridge,et al.  Testing the locality of transport in self-gravitating accretion discs , 2004 .

[11]  S. M. Fall,et al.  The Structure and Evolution of Normal Galaxies , 1981 .

[12]  P. Cassen,et al.  Evolution of Gravitationally Unstable Protostellar DIsks , 1991 .

[13]  Canada.,et al.  The Origin of Episodic Accretion Bursts in the Early Stages of Star Formation , 2005, astro-ph/0510014.

[14]  N. Turner,et al.  Turbulent Mixing and the Dead Zone in Protostellar Disks , 2006, astro-ph/0612552.

[15]  J. Najita,et al.  X-Ray Ionization of Protoplanetary Disks , 1997 .

[16]  R. Jayawardhana,et al.  Exploring brown dwarf disks : A 1.3 mm survey in taurus , 2006, astro-ph/0603619.

[17]  P. Cassen,et al.  The Effects of Thermal Energetics on Three-dimensional Hydrodynamic Instabilities in Massive Protostellar Disks , 1998 .

[18]  The role of the energy equation in the fragmentation of protostellar discs during stellar encounters , 2006, astro-ph/0610201.

[19]  L. Hartmann,et al.  Why Do T Tauri Disks Accrete? , 2006, astro-ph/0605294.

[20]  M. Norman,et al.  ZEUS-2D: A radiation magnetohydrodynamics code for astrophysical flows in two space dimensions. I - The hydrodynamic algorithms and tests. II - The magnetohydrodynamic algorithms and tests , 1992 .

[21]  K. Saigo,et al.  Similarity Solution for Formation of a Circumstellar Disk through the Collapse of a Flattened Rotating Cloud , 1998 .

[22]  Saeko S. Hayashi,et al.  Spiral Structure in the Circumstellar Disk around AB Aurigae , 2004 .

[23]  T. Henning,et al.  The Disk and Environment of the Herbig Be Star HD 100546 , 2001 .

[24]  L. Hartmann,et al.  Accretion processes in star formation , 1999 .

[25]  S. Weidenschilling The distribution of mass in the planetary system and solar nebula , 1977 .

[26]  S. Basu,et al.  THE BURST MODE OF PROTOSTELLAR ACCRETION , 2006, astro-ph/0607118.

[27]  Jonathan P. Williams,et al.  Circumstellar Dust Disks in Taurus-Auriga: The Submillimeter Perspective , 2005, astro-ph/0506187.

[28]  S. Tremaine,et al.  Galactic Dynamics , 2005 .

[29]  P. Bodenheimer,et al.  Nonaxisymmetric evolution in protostellar disks , 1994 .

[30]  Alyssa A. Goodman,et al.  Dense cores in dark clouds. VIII - Velocity gradients , 1993 .

[31]  D. Lynden-Bell,et al.  II. Spiral Arms as Sheared Gravitational Instabilities , 1965 .