Collision rate of bidisperse, hydrodynamically interacting spheres settling in a turbulent flow

2021 ◽  
Vol 912 ◽  
Author(s):  
Johnson Dhanasekaran ◽  
Anubhab Roy ◽  
Donald L. Koch

Abstract

1983 ◽  
Vol 9 (4) ◽  
pp. 421-435 ◽  
Author(s):  
J.J.E. Williams ◽  
R.I. Crane

2008 ◽  
Vol 65 (2) ◽  
pp. 357-374 ◽  
Author(s):  
M. Pinsky ◽  
A. Khain ◽  
H. Krugliak

Abstract The present study is a continuation of the series of studies dedicated to the investigation of cloud droplet collisions in turbulent flow with characteristics that are typical of real clouds. Detailed tables of collision kernels and collision efficiencies calculated in the presence of hydrodynamic interaction of droplets are presented. These tables were calculated for a wide range of turbulent parameters. To illustrate the sensitivity of droplet size distribution (DSD) evolution to the turbulence-induced increase in the collision rate, simulations of DSD evolution are preformed by solving the stochastic kinetic equation for collisions. The results can be applied to cloud modeling. The tables of collision efficiencies and collision kernels are available upon request. Some unsolved problems related to collisions of droplets and ice hydrometeors in turbulent clouds are discussed in the conclusion.


2002 ◽  
Vol 14 (8) ◽  
pp. 2921-2924 ◽  
Author(s):  
Z. Dodin ◽  
T. Elperin

2005 ◽  
Vol 62 (7) ◽  
pp. 2433-2450 ◽  
Author(s):  
Lian-Ping Wang ◽  
Orlando Ayala ◽  
Scott E. Kasprzak ◽  
Wojciech W. Grabowski

Abstract A methodology for conducting direct numerical simulations (DNSs) of hydrodynamically interacting droplets in the context of cloud microphysics has been developed and used to validate a new kinematic formulation capable of describing the collision rate and collision efficiency of cloud droplets in turbulent air. The theoretical formulation is formally the same as the formulation recently developed for geometrical collision rate of finite-inertia, nonsettling particles. It is shown that its application to hydrodynamically interacting droplets requires corrections because of a nonoverlap requirement. An approximate method for correcting the kinematic properties has been developed and validated against DNS data. The formulation presented here is more general and accurate than previously published formulations that, in most cases, are some extension to the description of hydrodynamic–gravitational collision. General dynamic and kinematic representations of the properly defined collision efficiency in a turbulent flow have been discussed. In addition to augmenting the geometric collision rate, air turbulence has been found to enhance the collision efficiency because, in a turbulent flow, hydrodynamic interactions become less effective in reducing the average relative radial velocity. The level of increase in the collision efficiency depends on the flow dissipation rate. For example, the collision efficiency between droplets of 20 and 25 μm in radii is increased by 59% and 10% by air turbulence at dissipation rates of 400 and 100 cm2 s−3, respectively. It is also shown that hydrodynamic interactions lead to higher droplet concentration fluctuations. The formulation presented here separates the effect of turbulence on collision efficiency from the previously observed effect of turbulence on the geometric collision rate.


2014 ◽  
Vol 749 ◽  
pp. 841-852 ◽  
Author(s):  
Michel Voßkuhle ◽  
Alain Pumir ◽  
Emmanuel Lévêque ◽  
Michael Wilkinson

AbstractTurbulence facilitates collisions between particles suspended in a turbulent flow. Two effects have been proposed that can enhance the collision rate at high turbulence intensities: ‘preferential concentration’ (a clustering phenomenon) and the ‘sling effect’ (arising from the formation of caustic folds in the phase space of the suspended particles). We have determined numerically the collision rate of small heavy particles as a function of their size and densities. The dependence on particle densities allows us to quantify the contribution of the sling effect to the collision rate. Our results demonstrate that the sling effect provides the dominant mechanism to the enhancement of the collision rate of particles, when inertia becomes significant.


1997 ◽  
Vol 158 (1) ◽  
pp. 201-230 ◽  
Author(s):  
F. E. KRUIS ◽  
K. A. KUSTERS

Author(s):  
Jean Mathieu ◽  
Julian Scott
Keyword(s):  

2021 ◽  
Vol 147 (3) ◽  
pp. 04020100
Author(s):  
Nasser Heydari ◽  
Panayiotis Diplas ◽  
J. Nathan Kutz ◽  
Soheil Sadeghi Eshkevari

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