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Influence of Saffman's lift force on the motion of a particle in a Couette layer
Authors:V A Naumov
Abstract:The article is concerned with the study of the effect of E. S. Asmolov's corrections to Saffman's lift force for the wall vicinity and a nonzero ratio of Reynolds numbers. It is shown in what way these corrections change the particle paths in a Couette layer and the conditions of deposition.Notation x=X/D, y=Y/D dimensionless longitudinal and transverse coordinates - u=U p /U infin, ngr=V p /U infin dimensionless projections of particle velocity on the longitudinal and transverse axes - tau=tU infin/D dimensionless time - U pardelta2/(18ngrlambdaD) Stokes number - lambda=rgr g /rgr p , ngr coefficient of the gas kinematic viscosity - delta particle diameter - 
$$\tilde \delta$$
delta/D - rgr g ,rgr p densities of the gas and particle material - 
$$\dot u$$
du/dtau - 
$$\dot v$$
dv/dtau - P s Saffman's force - C coefficient in the formula for Saffman's force - eegr yRe d 1/2 - A v r Re d 1/2 - agrzeta 3.08lambda - Rengr deltaV r /ngr - Re k delta2/ngr)partU g /partY - A Rengr/Re k 1/2 - Re d U infin D/ngr - V r ((U g –U p )2+V p 2 )1/2 Indices g refers to gas parameters - p refers to the parameters of particles - 0 at the time momentt=0 - S Saffman's force - k Reynolds number based on the velocity gradient - ngr based on velocity - r relative velocity - x projection on thex axis
Keywords:
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