2019
DOI: 10.1017/jfm.2019.865
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Turbophoresis of small inertial particles: theoretical considerations and application to wall-modelled large-eddy simulations

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Cited by 37 publications
(40 citation statements)
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References 85 publications
(106 reference statements)
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“…The particle phase is computed by advancing (2) with a second-order Runge-Kutta method, using trilinear interpolation to compute the fluid velocity at particle locations. Higher-order Lagrange interpolation schemes are tested and resulted in little change to the quantities of interest in this paper (Johnson et al, 2019). Particlewall collisions are computed using a unity restitution coefficient.…”
Section: Canonical Flow: Particle-laden Turbulent Channelmentioning
confidence: 99%
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“…The particle phase is computed by advancing (2) with a second-order Runge-Kutta method, using trilinear interpolation to compute the fluid velocity at particle locations. Higher-order Lagrange interpolation schemes are tested and resulted in little change to the quantities of interest in this paper (Johnson et al, 2019). Particlewall collisions are computed using a unity restitution coefficient.…”
Section: Canonical Flow: Particle-laden Turbulent Channelmentioning
confidence: 99%
“…The first term is the average wall-normal force on all particles at a particular distance from the wall. Using Stokes drag to illustrate the basic idea, a y |y = τ −1 p u y |y (recall that v y |y = 0 at steady-state), where u y |y > 0 as inertial particles tend to preferentially sample ejection events (Johnson, 2018;Johnson et al, 2019). This biased sampling of the flow leads to a net force on particles away from the wall.…”
Section: Turbophoresismentioning
confidence: 99%
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