Preferential concentration of particles by turbulence

1994 ◽  
Vol 20 ◽  
pp. 169-209 ◽  
Author(s):  
J.K. Eaton ◽  
J.R. Fessler
2003 ◽  
Vol 15 (6) ◽  
pp. 1776 ◽  
Author(s):  
Leonid I. Zaichik ◽  
Vladimir M. Alipchenkov

Author(s):  
M. Sato ◽  
M. Tanahashi ◽  
T. Miyauchi

Direct numerical simulations of homogeneous isotropic turbulence laden with particles have been conducted to clarify the relationship between particle dispersion and coherent fine scale eddies in turbulence. Dispersion of 106 particles are analyzed for several particle Stokes numbers. The spatial distributions of particles depend on their Stokes number, and the Stokes number that causes preferential concentration of particles is closely related to the time scale of coherent fine scale eddies in turbulence. On the plane perpendicular to the rotating axes of fine scale eddies, number density of particle with particular Stokes number is low at the center of the fine scale eddy, and high in the regions with high energy dissipation rate around the eddy. The maximum number density can be observed at about 1.5 to 2.0 times the eddy radius on the major axis of the fine scale eddy.


2003 ◽  
Author(s):  
Mikhael Gorokhovski ◽  
Anna Chtab

By analogy with kinetic approach, the gas-solid turbulent flow was considered as an ensemble of interacting both stochastic liquid and solid particles. In this way, the motion equation for the solid particle along a smoothed trajectory has been derived. To close this equation, the statistical temperature of particles has been introduced and expressed by statistical properties of turbulence. The smoothed particles dynamics was then computed along with large-eddy simulation (LES) of turbulent channel gas flow with “two-way” coupling of momentum. The calculated results are compared with the experiment of Kulick et. al. (1994) and with computation of Yamomoto et. al. (2001), where the inter-particle interaction has been simulated by hard-sphere collisions with prescribed efficiency. It has been shown that our computation with smoothed motion of particle is relatively in agreement with experiment and computations of Yamomoto et. al. (2001). At the same time, the model presented in the paper has a following advantage: it, practically, does not require an additional CPU time to account for inter-particle interactions. The turbulence attenuation by particles and the preferential concentration of particles in the low-turbulence region have been shown.


1994 ◽  
Vol 6 (11) ◽  
pp. 3742-3749 ◽  
Author(s):  
John R. Fessler ◽  
Jonathan D. Kulick ◽  
John K. Eaton

2014 ◽  
Vol 15 (5) ◽  
pp. 293-310 ◽  
Author(s):  
Martín Obligado ◽  
Tomás Teitelbaum ◽  
Alain Cartellier ◽  
Pablo Mininni ◽  
Mickaël Bourgoin

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