Lagrangian Flow Geometry of Tripolar Vortex

Author(s):  
Lorena A. Barba ◽  
Oscar U. Velasco Fuentes
2008 ◽  
Vol 38 (12) ◽  
pp. 2817-2831 ◽  
Author(s):  
M. Duran-Matute ◽  
O. U. Velasco Fuentes

Abstract The flow of a vortex advected by a uniform current toward a gap in a straight barrier is studied. This is an idealization of flows observed in the world’s oceans, for example, in the Yucatan Channel and in the various passages of the Lesser Antilles. The vortex evolution and the transport properties are studied as a function of three nondimensional parameters related to the vortex intensity, the vortex initial position, and the gap’s span. The flow evolution is computed numerically with a two-dimensional inviscid model. The vortex is observed to behave in one of the following ways: it passes completely through the gap, it splits and only a fraction passes, or it stays entirely in the upstream side of the wall. In each of these regimes, transport and mixing are analyzed using the Lagrangian flow geometry, finite-size Lyapunov exponents, and residence times of fluid particles. Laboratory experiments are performed in a homogeneous, rotating fluid. In the region of parameter space that leads to total passage of the vortex, there is good agreement between the evolution observed in the laboratory and that obtained numerically. In the regions of parameter space, which lead to partial passage and full blockage, the agreement is good only until the generation of vorticity on the walls becomes important.


2021 ◽  
Vol 154 ◽  
pp. 105758
Author(s):  
Dániel Megyeri ◽  
Attila Kohut ◽  
Zsolt Geretovszky

2018 ◽  
Vol 108 ◽  
pp. 80-92
Author(s):  
Ricardo Medina ◽  
Russell L. Detwiler ◽  
Romain Prioul ◽  
Wenyue Xu ◽  
Jean E. Elkhoury

2011 ◽  
Vol 23 (12) ◽  
pp. 125107 ◽  
Author(s):  
Y. Minamoto ◽  
N. Fukushima ◽  
M. Tanahashi ◽  
T. Miyauchi ◽  
T. D. Dunstan ◽  
...  

2006 ◽  
Vol 128 (4) ◽  
pp. 874-879 ◽  
Author(s):  
Roberto C. Aguirre ◽  
Jennifer C. Nathman ◽  
Haris C. Catrakis

Flow geometry effects are examined on the turbulent mixing efficiency quantified as the mixture fraction. Two different flow geometries are compared at similar Reynolds numbers, Schmidt numbers, and growth rates, with fully developed turbulence conditions. The two geometries are the round jet and the single-stream planar shear layer. At the flow conditions examined, the jet exhibits an ensemble-averaged mixing efficiency which is approximately double the value for the shear layer. This substantial difference is explained fluid mechanically in terms of the distinct large-scale entrainment and mixing-initiation environments and is therefore directly due to flow geometry effects.


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