The coagulation equation has been widely used to describe various kinds of accretion processes. Owing to its statistical property, however, the coagulation equation has a serious defect in some cases, i.e., sometimes the total mass of a system is not conserved. The aim of the present study is to fin
The Timescale of Runaway Stochastic Coagulation
β Scribed by Leonid Malyshkin; Jeremy Goodman
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 121 KB
- Volume
- 150
- Category
- Article
- ISSN
- 0019-1035
No coin nor oath required. For personal study only.
β¦ Synopsis
We study the stochastic coagulation equation using simplified models and efficient Monte Carlo simulations. It is known that (i) runaway growth occurs if the two-body coalescence kernel rises faster than linearly in the mass of the heavier particle; and (ii) for such kernels, runaway is instantaneous in the limit that the number of particles tends to infinity at fixed collision time per particle. Superlinear kernels arise in astrophysical systems where gravitational focusing is important, such as the coalescence of planetesimals to form planets or of stars to form supermassive black holes. We find that the time for all particles to coalesce into a single body decreases as a power of the logarithm of the initial number of particles. Astrophysical implications are briefly discussed.
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The coagulation equation, which is widely used for modeling growth in planet formation and other astrophysical problems, is the mean-rate equation that describes the evolution of the mass spectrum of a collection of particles due to successive mergers. A numerical code that can yield accurate soluti
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