Dust coagulation and fragmentation in molecular clouds I. How collisions between dust aggregates alter the dust size distribution

被引:209
|
作者
Ormel, C. W. [1 ,2 ]
Paszun, D. [3 ]
Dominik, C. [3 ,4 ]
Tielens, A. G. G. M. [5 ,6 ]
机构
[1] Univ Groningen, Kapteyn Astron Inst, NL-9700 AV Groningen, Netherlands
[2] Max Planck Inst Astron, D-69117 Heidelberg, Germany
[3] Sterrenkundig Inst Anton Pannekoek, NL-1098 SJ Amsterdam, Netherlands
[4] Radboud Univ Nijmegen, Afdeling Sterrenkunde, NL-6500 GL Nijmegen, Netherlands
[5] NASA, Ames Res Ctr, Moffett Field, CA 94035 USA
[6] Leiden Univ, Leiden Observ, NL-2300 RA Leiden, Netherlands
关键词
ISM: dust; extinction; ISM: clouds; turbulence; methods: numerical; HEAD-ON COLLISIONS; 2 ELASTIC SPHERES; STAR-FORMATION; PROTOPLANETARY DISKS; OPTICAL-PROPERTIES; INTERSTELLAR DUST; MU-M; WAVELENGTH DEPENDENCE; NUMERICAL-SIMULATION; PROTOSTELLAR CORES;
D O I
10.1051/0004-6361/200811158
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The cores in molecular clouds are the densest and coldest regions of the interstellar medium (ISM). In these regions ISM-dust grains have the potential to coagulate. This study investigates the collisional evolution of the dust population by combining two models: a binary model that simulates the collision between two aggregates and a coagulation model that computes the dust size distribution with time. In the first, results from a parameter study quantify the outcome of the collision - sticking, fragmentation (shattering, breakage, and erosion) - and the effects on the internal structure of the particles in tabular format. These tables are then used as input for the dust evolution model, which is applied to an homogeneous and static cloud of temperature 10 K and gas densities between 10(3) and 10(7) cm(-3). The coagulation is followed locally on timescales of similar to 10(7) yr. We find that the growth can be divided into two stages: a growth dominated phase and a fragmentation dominated phase. Initially, the mass distribution is relatively narrow and shifts to larger sizes with time. At a certain point, dependent on the material properties of the grains as well as on the gas density, collision velocities will become sufficiently energetic to fragment particles, halting the growth and replenishing particles of lower mass. Eventually, a steady state is reached, where the mass distribution is characterized by a mass spectrum of approximately equal amount of mass per logarithmic size bin. The amount of growth that is achieved depends on the cloud's lifetime. If clouds exist on free-fall timescales the effects of coagulation on the dust size distribution are very minor. On the other hand, if clouds have long-term support mechanisms, the impact of coagulation is important, resulting in a significant decrease of the opacity on timescales longer than the initial collision timescale between big grains.
引用
收藏
页码:845 / 869
页数:25
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