Stochastic dynamics of particles trapped in turbulent flows

The long-time dynamics of large particles trapped in two nonhomogeneous turbulent shear flows is studied experimentally. Both flows present a common feature, a shear region that separates two colliding circulations, but with different spatial symmetries and temporal behaviors. Because large particle...

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Detalles Bibliográficos
Autores: Machicoane, N. (N.)|||/items/e4ace788-09d9-4a64-885b-83ab97a17386, Lopez-Caballero, M. (Miguel)|||/items/50e7b5df-ee8b-4a85-ab51-3010fbb22254, Fiabane, L. (L)|||/items/9a4e1180-fc90-4ea2-be93-2fa26e752cc0, Pinton, J.F. (Jean-François)|||/items/b4f37a53-a32b-4313-bc21-4136286f1c46, Bourgoin, M. (M.)|||/items/4e4afd2d-7d02-4f48-8436-c6f920f7e363, Burguete-Mas, F.J. (Francisco Javier)|||/items/408b1397-b3d1-4939-a7f3-e673d3a80721, Volk, R. (R.)|||/items/4ecc0d79-2245-42ef-8319-12b798ded00c
Tipo de recurso: artículo
Fecha de publicación:2016
País:España
Institución:Universidad de Navarra
Repositorio:Dadun. Depósito Académico Digital de la Universidad de Navarra
Idioma:inglés
OAI Identifier:oai:dadun.unav.edu:10171/40164
Acceso en línea:https://hdl.handle.net/10171/40164
Access Level:acceso abierto
Palabra clave:Particles
Stochastic dynamics
Turbulent flows
Descripción
Sumario:The long-time dynamics of large particles trapped in two nonhomogeneous turbulent shear flows is studied experimentally. Both flows present a common feature, a shear region that separates two colliding circulations, but with different spatial symmetries and temporal behaviors. Because large particles are less and less sensitive to flow fluctuations as their size increases, we observe the emergence of a slow dynamics corresponding to back-and-forth motions between two attractors, and a super-slow regime synchronized with flow reversals when they exist. Such dynamics is substantially reproduced by a one-dimensional stochastic model of an overdamped particle trapped in a two-well potential, forced by a colored noise. An extended model is also proposed that reproduces observed dynamics and trapping without potential barrier: the key ingredient is the ratio between the time scales of the noise correlation and the particle dynamics. A total agreement with experiments requires the introduction of spatially nonhomogeneous fluctuations and a suited confinement strength.