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Stokes flow paths separation and recirculation cells in X-junctions of varying angle

Authors :
Jean-Pierre Hulin
J. M. Gomba
M. Cachile
Harold Auradou
Laurent Talon
Grupo de Medios Porosos [Buenos Aires] (GMP)
Facultad de Ingeniería [Buenos Aires] (FIUBA)
Universidad de Buenos Aires [Buenos Aires] (UBA)-Universidad de Buenos Aires [Buenos Aires] (UBA)
Fluides, automatique, systèmes thermiques (FAST)
Université Paris-Sud - Paris 11 (UP11)-Université Pierre et Marie Curie - Paris 6 (UPMC)-Centre National de la Recherche Scientifique (CNRS)
Instituto de Física Arroyo Seco [Tandil] (IFAS)
Facultad de Ciencias Exactas [Tandil]
Universidad Nacional del Centro de la Provincia de Buenos Aires [Buenos Aires] (UNICEN)-Universidad Nacional del Centro de la Provincia de Buenos Aires [Buenos Aires] (UNICEN)
RTRA 'Triangle de la Physique'
LIA PMF-FMF (Franco-Argentinian International Associated Laboratory in the Physics and Mechanics of Fluids).
Source :
Physics of Fluids, Physics of Fluids, American Institute of Physics, 2012, 24 (2), pp.021704. ⟨10.1063/1.3690100⟩, CONICET Digital (CONICET), Consejo Nacional de Investigaciones Científicas y Técnicas, instacron:CONICET, Physics of Fluids, 2012, 24 (2), pp.021704. ⟨10.1063/1.3690100⟩
Publication Year :
2012
Publisher :
HAL CCSD, 2012.

Abstract

Fluid and solute transfer in X-junctions between straight channels is shown to depend critically on the junction angle α in the Stokes flow regime. Experimentally, water and a water-dye solution are injected at equal flow rates in two facing channels of the junction. Planar laser induced fluorescence (PLIF) measurements show that the largest part of each injected fluid "bounces back" preferentially into the outlet channel at the lowest angle to the injection; this is opposite to the inertial case and requires a high curvature of the corresponding streamlines. The proportion of this fluid in the other channel decreases from 50% at α = 90° to 0% at a threshold angle. These counterintuitive features reflect the minimization of energy dissipation for Stokes flows. Finite elements numerical simulations of a 2D Stokes flow of equivalent geometry confirm these results and show that, below the threshold angle αc = 33.8°, recirculation cells are present in the center part of the junction and separate the two injected flows of the two solutions. Reducing further α leads to the appearance of new recirculation cells with lower flow velocities. Fil: Cachile, Mario Andres. Universidad de Buenos Aires. Facultad de Ingeniería. Departamento de Física. Grupo de Medios Porosos; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina Fil: Talon, L.. Universite de Paris Xi. Laboratoire Automatiques et Systeme Thermiques; Francia Fil: Gomba, Juan Manuel. Universidad Nacional del Centro de la Provincia de Buenos Aires. Facultad de Ciencias Exactas. Instituto de Fisica Arroyo Seco; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina Fil: Hulin, J.P.. Universite de Paris Xi. Laboratoire Automatiques et Systeme Thermiques; Francia Fil: Auradou, H.. Universite de Paris Xi. Laboratoire Automatiques et Systeme Thermiques; Francia

Details

Language :
English
ISSN :
10706631 and 10897666
Database :
OpenAIRE
Journal :
Physics of Fluids, Physics of Fluids, American Institute of Physics, 2012, 24 (2), pp.021704. ⟨10.1063/1.3690100⟩, CONICET Digital (CONICET), Consejo Nacional de Investigaciones Científicas y Técnicas, instacron:CONICET, Physics of Fluids, 2012, 24 (2), pp.021704. ⟨10.1063/1.3690100⟩
Accession number :
edsair.doi.dedup.....26f6b7f65529dfd25bd9da2900354665
Full Text :
https://doi.org/10.1063/1.3690100⟩