2019
DOI: 10.1063/1.5119103
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Particles in turbulent separated flow over a bump: Effect of the Stokes number and lift force

Abstract: Particle-laden turbulent flow that separates due to a bump inside a channel is simulated to analyse the effects of the Stokes number and the lift force on the particle spatial distribution. The fluid friction Reynolds number is approximately 900 over the bump, the highest achieved for similar computational domains. A range of particle Stokes numbers are considered, each simulated with and without the lift force in the particle dynamic equation. When the lift force is included a significant difference in the pa… Show more

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Cited by 17 publications
(5 citation statements)
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“…dissipation of turbulent kinetic energy were analysed via the generalized Kolmogorov equation. In Mollicone et al (2019) a similar set-up, with a smooth bump defined by a cosine function, was used to study particle-laden flows at finite values of the Stokes number.…”
Section: Introductionmentioning
confidence: 99%
“…dissipation of turbulent kinetic energy were analysed via the generalized Kolmogorov equation. In Mollicone et al (2019) a similar set-up, with a smooth bump defined by a cosine function, was used to study particle-laden flows at finite values of the Stokes number.…”
Section: Introductionmentioning
confidence: 99%
“…( 9) .Here, 𝜏𝜏 p denotes the particle response time, and 𝜏𝜏 f stands for the characteristic response time of the fluid. However, high Stokes number indicates that particles exhibit more inertia-driven behaviour and are less affected by fluid flow [28].However, the continuum description of the fluid phase is justified based on Knudsen number , in our specific case, stands at a value of 0.001. Consequently, no slip-boundary effects are observed at the interface between the fluid and particle phases.…”
Section: Resultsmentioning
confidence: 86%
“…The presence of flow confinement introduces additional complexity. The preferential segregation of the particles near the walls [10][11][12] leads the particles to a↵ect the turbulence in the bu↵er-layer 13 . It follows a modification of the regeneration cycle of the vortical structures, and of the flow topology [14][15][16][17] , which ultimately manifests, at least for finite-size neutrally buoyant particles, in a modification of the well-known law of the wall 18 .…”
Section: Introductionmentioning
confidence: 99%