Gustavsson, K.; Mehlig, B. and Wilkinson, M.
|DOI (Digital Object Identifier) Link:||http://doi.org/10.1088/1367-2630/10/7/075014|
|Google Scholar:||Look up in Google Scholar|
We consider collisions of particles advected in a fluid. As already pointed out by Smoluchowski (1917 Z. Phys. Chem. 92 129–68), macroscopic motion of the fluid can significantly enhance the frequency of collisions between the suspended particles. This effect was invoked by Saffman and Turner (1956 J. Fluid Mech. 1 16–30) to estimate collision rates of small water droplets in turbulent rain clouds, the macroscopic motion being caused by turbulence. Here, we show that the Saffman–Turner theory is unsatisfactory because it describes an initial transient only. The reason for this failure is that the local flow in the vicinity of a particle is treated as if it were a steady hyperbolic flow, whereas, in reality, it must fluctuate. We derive exact expressions for the steady-state collision rate for particles suspended in rapidly fluctuating random flows and compute how this steady state is approached. For incompressible flows, the Saffman–Turner expression is an upper bound.
|Item Type:||Journal Article|
|Copyright Holders:||2008 Institute of Physics|
|Academic Unit/Department:||Faculty of Science, Technology, Engineering and Mathematics (STEM) > Mathematics and Statistics
Faculty of Science, Technology, Engineering and Mathematics (STEM)
|Depositing User:||Michael Wilkinson|
|Date Deposited:||11 Dec 2010 17:45|
|Last Modified:||02 Aug 2016 13:53|
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