1995
DOI: 10.1063/1.868778
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Dynamics of heavy particles in a Burgers vortex

Abstract: This paper presents a linear stability analysis as well as some numerical results for the motion of heavy particles in the flow field of a Burgers vortex, under the combined effects of particle inertia, Stokes drag, and gravity. By rendering the particle motion equations dimensionless, the particle Stokes number, a Froude number, and a vortex Reynolds number are obtained as the governing three parameters. In the absence of gravity, the vortex center represents a stable equilibrium point for particles up to a c… Show more

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Cited by 56 publications
(44 citation statements)
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“…Very small particles may not have steady-state orbits, instead they reach the tube center because of the efficient radial drag. The steady-state radius, which we will refer to as the equilibrium radius, can be estimated from the equation u 2 θ /r = Ar/τ p (Marcu et al 1995). Using u θ as a function of r in Equation (A1), we see that larger friction timescales give larger equilibrium radii.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Very small particles may not have steady-state orbits, instead they reach the tube center because of the efficient radial drag. The steady-state radius, which we will refer to as the equilibrium radius, can be estimated from the equation u 2 θ /r = Ar/τ p (Marcu et al 1995). Using u θ as a function of r in Equation (A1), we see that larger friction timescales give larger equilibrium radii.…”
Section: Discussionmentioning
confidence: 99%
“…As it moves closer to the center, the particle rotates faster. When the centrifugal force from the rotation balances the radial drag, the particle ends up in a steadystate orbit (Marcu et al 1995). Very small particles may not have steady-state orbits, instead they reach the tube center because of the efficient radial drag.…”
Section: Discussionmentioning
confidence: 99%
“…The result is a modified velocity field, whose fixed points represent equilibrium points for the particles. 20 In the absence of gravity, the streamlines of this modified velocity field are identical to the streamlines of the fluid velocity field, shown in Fig. 1͑b͒ for kϭ0.9 and ϭ4.…”
Section: A Gravity Perpendicular To the Mixing Layermentioning
confidence: 66%
“…1, so that they are unstable for particle accumulation. 20 In the following, we analyze the linear stability at the center of the vortex located at zϭ0. 25, yϭ0.…”
Section: Equilibrium Points and Their Stability In The Absence Omentioning
confidence: 99%
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