EFFECT OF NONLINEAR DRAG ON THE SETTLING VELOCITY OF PARTICLES IN HOMOGENEOUS ISOTROPIC TURBULENCE

Authors
Citation
Jch. Fung, EFFECT OF NONLINEAR DRAG ON THE SETTLING VELOCITY OF PARTICLES IN HOMOGENEOUS ISOTROPIC TURBULENCE, J GEO RES-O, 103(C12), 1998, pp. 27905-27917
Citations number
34
Categorie Soggetti
Oceanografhy,"Geosciences, Interdisciplinary","Astronomy & Astrophysics","Geochemitry & Geophysics","Metereology & Atmospheric Sciences
Journal title
JOURNAL OF GEOPHYSICAL RESEARCH-OCEANS
ISSN journal
21699275 → ACNP
Volume
103
Issue
C12
Year of publication
1998
Pages
27905 - 27917
Database
ISI
SICI code
2169-9275(1998)103:C12<27905:EONDOT>2.0.ZU;2-N
Abstract
We study the average settling velocity of small spherical particles un der gravity through a Gaussian random velocity field generated by Four ier modes with a von Karman energy spectrum. The particles are subject ed to the effects of a linear (Stokes) or nonlinear drag force, inerti a and gravity. It is shown that the effect of drag nonlinearity is a f unction of the particle to fluid density ratio rho(p)/rho(f) and a fun ction of the ratio tau(p)/tau(k) Of the particle time constant to the Kolmogorov timescale of the fluid. Simulations show that as rho(p)/rho (f) decreases from 877 to 2.65 or as tau(p)/tau(k) increases from 1 to 2.74, the drag nonlinearity increases as a result oi the increase in particle Reynolds numbers. Hence the settling velocity changes from la rger to smaller as compared with the still fluid settling velocity, sh owing that one of the major mechanisms governing the fall velocity red uction in a turbulent flow is the drag nonlinearity. The maximum incre ase in settling rate occurs at V-T/upsilon(k) approximate to 2 for rho (p)/rho(f) greater than or equal to 87 (where V-T is the terminal velo city of the particle and upsilon(k) is the Kolmogorov velocity); this is consistent with the results of Wang and Maxey [1993]. The maximum d ecrease in settling rate occurs at V-T/upsilon(k) approximate to 1 for rho(p)/rho(f) approximate to 2.65, consistent with the results of Fun g [1993]. In addition, the role of the spatial and temporal variations of the flow field on the settling rate is investigated. Finally, the Gaussian velocity field is also simulated with an exponential energy s pectrum, and similar results are observed.