Gravitational Collapse in Turbulent Molecular Clouds. I. Gasdynamical Turbulence

Observed molecular clouds often appear to have very low star formation efficiencies and lifetimes an order of magnitude longer than their free-fall times. Their support is attributed to the random supersonic motions observed in them. We study the support of molecular clouds against gravitational collapse by supersonic, gasdynamical turbulence using direct numerical simulation. Computations with two different algorithms are compared: a particle-based, Lagrangian method (smoothed particle hydrodynamics [SPH]) and a grid-based, Eulerian, second-order method (ZEUS). The effects of both algorithm and resolution can be studied with this method. We find that, under typical molecular cloud conditions, global collapse can indeed be prevented, but density enhancements caused by strong shocks nevertheless become gravitationally unstable and collapse into dense cores and, presumably, stars. The occurrence and efficiency of local collapse decreases as the driving wavelength decreases and the driving strength increases. It appears that local collapse can be prevented entirely only with unrealistically short wavelength driving, but observed core formation rates can be reproduced with more realistic driving. At high collapse rates, cores are formed on short timescales in coherent structures with high efficiency, while at low collapse rates they are scattered randomly throughout the region and exhibit considerable age spread. We suggest that this naturally explains the observed distinction between isolated and clustered star formation.

[1]  R. Klessen One-Point Probability Distribution Functions of Supersonic Turbulent Flows in Self-gravitating Media , 2000, astro-ph/0001379.

[2]  B. Elmegreen Star Formation in a Crossing Time , 1999, astro-ph/9911172.

[3]  R. Klessen,et al.  The Formation of Stellar Clusters: Gaussian Cloud Conditions. I. , 1999, astro-ph/9904090.

[4]  A. Boss,et al.  Protostars and Planets VI , 2000 .

[5]  Fernández,et al.  Allergy to the pine processionary caterpillar (Thaumetopoea pityocampa) , 1999, Clinical and experimental allergy : journal of the British Society for Allergy and Clinical Immunology.

[6]  L. Hartmann,et al.  Turbulent Flow-driven Molecular Cloud Formation: A Solution to the Post-T Tauri Problem? , 1999, astro-ph/9907053.

[7]  P. Padoan,et al.  A Super-Alfvénic Model of Dark Clouds , 1999, astro-ph/9901288.

[8]  James M. Stone,et al.  Kinetic and Structural Evolution of Self-gravitating, Magnetized Clouds: 2.5-Dimensional Simulations of Decaying Turbulence , 1998, astro-ph/9810321.

[9]  J. Scalo,et al.  Clouds as Turbulent Density Fluctuations: Implications for Pressure Confinement and Spectral Line Data Interpretation , 1998, astro-ph/9806059.

[10]  E. Grebel,et al.  Some Characteristics of Current Star Formation in the 30 Doradus Nebula Revealed by HST/NICMOS , 1999 .

[11]  Eve C. Ostriker Interstellar Turbulence: The Evolution of Self-Gravitating, Magnetized, Turbulent Clouds: Numerical Experiments , 1999 .

[12]  Richard M. Crutcher,et al.  Magnetic Fields in Molecular Clouds: Observations Confront Theory , 1998 .

[13]  E. Ostriker,et al.  Dissipation in Compressible Magnetohydrodynamic Turbulence , 1998, astro-ph/9809357.

[14]  M. M. Low The Energy Dissipation Rate of Supersonic, Magnetohydrodynamic Turbulence in Molecular Clouds , 1998, astro-ph/9809177.

[15]  L. Hillenbrand,et al.  A Preliminary Study of the Orion Nebula Cluster Structure and Dynamics , 1998 .

[16]  R. Klessen,et al.  Kinetic Energy Decay Rates of Supersonic and Super-Alfvénic Turbulence in Star-Forming Clouds , 1997, astro-ph/9712013.

[17]  R. Klessen,et al.  Fragmentation of Molecular Clouds: The Initial Phase of a Stellar Cluster , 1997, astro-ph/9710318.

[18]  S. Lizano,et al.  Does Turbulent Pressure Behave as a Logatrope? , 1997, astro-ph/9708148.

[19]  Richard I. Klein,et al.  The Jeans Condition: A New Constraint on Spatial Resolution in Simulations of Isothermal Self-Gravitational Hydrodynamics , 1997 .

[20]  M. Bate,et al.  Resolution requirements for smoothed particle hydrodynamics calculations with self-gravity , 1997 .

[21]  L. Hillenbrand On the Stellar Population and Star-Forming History of the Orion Nebula Cluster , 1997 .

[22]  R. Klessen GRAPESPH with fully periodic boundary conditions: fragmentation of molecular clouds , 1997, astro-ph/9704004.

[23]  E. Zweibel,et al.  Current Sheet Formation in the Interstellar Medium , 1997 .

[24]  M. Heyer,et al.  Application of Principal Component Analysis to Large-Scale Spectral Line Imaging Studies of the Interstellar Medium , 1997 .

[25]  Sánchez,et al.  Fractal dimensions and scaling laws in the interstellar medium: A new field theory approach. , 1996, Physical review. D, Particles and fields.

[26]  F. Combes,et al.  Self-gravity as an explanation of the fractal structure of the interstellar medium , 1996, Nature.

[27]  T. Passot,et al.  Influence of Cooling-Induced Compressibility on the Structure of Turbulent Flows and Gravitational Collapse , 1996, astro-ph/9607046.

[28]  E. Ostriker,et al.  Can Nonlinear Hydromagnetic Waves Support a Self-gravitating Cloud? , 1996, astro-ph/9601095.

[29]  M. Steinmetz Grapesph: cosmological smoothed particle hydrodynamics simulations with the special-purpose hardware GRAPE , 1995, astro-ph/9504050.

[30]  I. Bonnell,et al.  Modelling accretion in protobinary systems , 1995, astro-ph/9510149.

[31]  Y. Fukui,et al.  Overall Distribution of Dense Molecular Gas and Star Formation in the Taurus Cloud Complex , 1995 .

[32]  T. Passot,et al.  A turbulent model for the interstellar medium. I. Threshold star formation and self-gravity , 1995 .

[33]  T. Passot,et al.  A Turbulent Model for the Interstellar Medium. II. Magnetic Fields and Rotation , 1994, astro-ph/9601182.

[34]  M. Norman,et al.  Shock interactions with magnetized interstellar clouds. 1: Steady shocks hitting nonradiative clouds , 1994 .

[35]  Leo Blitz,et al.  DETERMINING STRUCTURE IN MOLECULAR CLOUDS , 1994 .

[36]  Paul R. Woodward,et al.  Kolmogorov‐like spectra in decaying three‐dimensional supersonic flows , 1994 .

[37]  R. Klein,et al.  On the hydrodynamic interaction of shock waves with interstellar clouds. 1: Nonradiative shocks in small clouds , 1994 .

[38]  B. Elmegreen Star Formation at Compressed Interfaces in Turbulent Self-gravitating Clouds , 1993 .

[39]  J. Monaghan Smoothed particle hydrodynamics , 2005 .

[40]  M. Pérault,et al.  Jeans collapse of turbulent gas clouds: tentative theory , 1992, Journal of Fluid Mechanics.

[41]  Paul R. Woodward,et al.  A numerical study of supersonic turbulence , 1992 .

[42]  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 .

[43]  Porter,et al.  Three-dimensional supersonic homogeneous turbulence: A numerical study. , 1992, Physical review letters.

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

[45]  T. Mouschovias Cosmic Magnetism and the Basic Physics of the Early Stages of Star Formation , 1991 .

[46]  C. Lada,et al.  Book-Review - the Physics of Star Formation and Early Stellar Evolution , 1991 .

[47]  Toshikazu Ebisuzaki,et al.  A special-purpose computer for gravitational many-body problems , 1990, Nature.

[48]  J. R. Buchler,et al.  The numerical modelling of nonlinear stellar pulsations: problems and prospects. Proceedings. , 1990 .

[49]  J. Robert Buchler,et al.  The Numerical Modelling of Nonlinear Stellar Pulsations , 1990 .

[50]  W. Benz Smooth Particle Hydrodynamics: A Review , 1990 .

[51]  A. Pouquet,et al.  Influence of supersonic turbulence on self-gravitating flows , 1990 .

[52]  D. Leisawitz Physical Properties of the Molecular Clouds Found in a CO Survey of Regions Around 34 Open Clusters , 1989 .

[53]  M. S. Matthews,et al.  Protostars & planets II , 1985 .

[54]  J. Monaghan,et al.  Shock simulation by the particle method SPH , 1983 .

[55]  E. Zweibel,et al.  Hydromagnetic wave dissipation in molecular clouds , 1983 .

[56]  C. Lada,et al.  Star formation in the lambda orionis region. I. The distribution of young objects , 1982 .

[57]  L. Blitz,et al.  THE ORIGIN AND LIFETIME OF GIANT MOLECULAR CLOUD COMPLEXES , 1980 .

[58]  R. Larson Turbulence and star formation in molecular clouds , 1980 .

[59]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme. IV. A new approach to numerical convection , 1977 .

[60]  S. Chandrasekhar The gravitational instability of an infinite homogeneous turbulent medium , 1951, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[61]  V. Weizsäcker The Evolution of Galaxies and Stars. , 1951 .

[62]  James Jeans,et al.  The stability of a spherical Nebula , 1901, Proceedings of the Royal Society of London.

[63]  Seung Choi,et al.  ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? J ? ? J ? ? ? ? ? ? ? ? ? ? ? ? ? ? , 2022 .