Numerical Modelling of Two-Dimensional Flow Patterns in Shallow Rectangular Basins

2013 ◽  
pp. 499-510 ◽  
Author(s):  
Matthieu Secher ◽  
Jean-Michel Hervouet ◽  
Pablo Tassi ◽  
Eric Valette ◽  
Catherine Villaret
2011 ◽  
Vol 278 (1725) ◽  
pp. 3670-3678 ◽  
Author(s):  
Brooke E. Flammang ◽  
George V. Lauder ◽  
Daniel R. Troolin ◽  
Tyson Strand

Understanding how moving organisms generate locomotor forces is fundamental to the analysis of aerodynamic and hydrodynamic flow patterns that are generated during body and appendage oscillation. In the past, this has been accomplished using two-dimensional planar techniques that require reconstruction of three-dimensional flow patterns. We have applied a new, fully three-dimensional, volumetric imaging technique that allows instantaneous capture of wake flow patterns, to a classic problem in functional vertebrate biology: the function of the asymmetrical (heterocercal) tail of swimming sharks to capture the vorticity field within the volume swept by the tail. These data were used to test a previous three-dimensional reconstruction of the shark vortex wake estimated from two-dimensional flow analyses, and show that the volumetric approach reveals a different vortex wake not previously reconstructed from two-dimensional slices. The hydrodynamic wake consists of one set of dual-linked vortex rings produced per half tail beat. In addition, we use a simple passive shark-tail model under robotic control to show that the three-dimensional wake flows of the robotic tail differ from the active tail motion of a live shark, suggesting that active control of kinematics and tail stiffness plays a substantial role in the production of wake vortical patterns.


2011 ◽  
Vol 26 (15) ◽  
pp. 2225-2234 ◽  
Author(s):  
Dalmo A. N. Vieira ◽  
Seth M. Dabney

2011 ◽  
Vol 23 (9) ◽  
pp. 091104 ◽  
Author(s):  
Mohamed Fayed ◽  
Rocco Portaro ◽  
Amy-Lee Gunter ◽  
Hamid Ait Abderrahmane ◽  
Hoi Dick Ng

1971 ◽  
Vol 50 (1) ◽  
pp. 177-188 ◽  
Author(s):  
Kathleen Trustrum

The Oseen equations for the two-dimensional flow of a Boussinesq fluid over a thin barrier placed in a channel of finite depth are solved in the double limit ν → 0, t → ∞ under the hypothesis that the velocity at the tip of the barrier is as weakly singular as possible. The predicted flow patterns and drag coefficients are in closer agreement with Davis's experimental observations than those of the Long model.


1999 ◽  
Vol 2 (3) ◽  
pp. 251-262
Author(s):  
P. Gestoso ◽  
A. J. Muller ◽  
A. E. Saez

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