Flow structure and scaling laws in lateral wing-tip blowing

AIAA Journal ◽  
1989 ◽  
Vol 27 (8) ◽  
pp. 1002-1007 ◽  
Author(s):  
C. S. Lee ◽  
D. Tavella ◽  
N. J. Wood ◽  
L. Roberts
1986 ◽  
Author(s):  
C. LEE ◽  
D. TAVELLA ◽  
N. WOOD ◽  
L. ROBERTS
Keyword(s):  

1999 ◽  
Vol 394 ◽  
pp. 357-377 ◽  
Author(s):  
WILLIAM J. DEVENPORT ◽  
CHRISTINE M. VOGEL ◽  
JEFFERY S. ZSOLDOS

Experiments have been performed to study the co-rotating wing-tip vortex pair produced by a pair of rectangular wings in a split-wing configuration. Detailed measurements made in cross-sections upstream and downstream of merger reveal, for the first time, the complex turbulence structure of this flow. The vortices spiral around each other and merge some 20 chordlengths downstream of the wings. As merger is approached the vortices lose their axisymmetry – their cores develop lopsided tangential velocity fields and the mean vorticity field is convected into filaments. The cores also become part of a single turbulence structure dominated by a braid of high turbulence levels that links them together. The braid, which quite closely resembles the structure formed between adjacent spanwise eddies of transitional mixing layers, grows in intensity with downstream distance and extends into the vortex cores. Unlike a single tip vortex, the unmerged cores appear turbulent.The merging of the vortices wraps the cores and the flow structure that surrounds them into a large turbulent region with an intricate double spiral structure. This structure then relaxes to a closely axisymmetric state. The merged core appears stable and develops a structure similar to the laminar core of a vortex shed from a single wing. However, the turbulent region formed around the vortex core during the merger process is much larger and more axisymmetric than that found around a single wing-tip vortex.


1988 ◽  
Vol 25 (4) ◽  
pp. 311-316 ◽  
Author(s):  
D. A. Tavella ◽  
N. J. Wood ◽  
C. S. Lee ◽  
L. Roberts
Keyword(s):  

1998 ◽  
Vol 120 (1) ◽  
pp. 234-242 ◽  
Author(s):  
D. Gobin ◽  
B. Goyeau ◽  
J.-P. Songbe

This study deals with natural convection driven by combined thermal and solutal buoyancy forces in a binary fluid. The consequence of thermosolutal convection on heat and mass transfer is examined in a confined enclosure partially filled with a porous medium. The mathematical description of the problem makes use of a one-domain formulation of the conservation equations. The presented numerical results quantitatively show the significant influence of the presence of a relatively thin porous layer on the flow structure and on heat and species transfer in the enclosure. The paper is dedicated to the analysis of the influence of the thickness and permeability of the porous layer in a range of governing parameters. For a low permeability porous layer, the numerical results are compared to an analysis based on simple scaling laws, which provide a good interpretation in terms of the wall transfer decrease with the porous layer thickness. The effect of permeability is investigated and it is shown that flow penetration in the porous layer induces a specific behavior of the flow structure and average heat transfer in the enclosure.


1994 ◽  
Vol 144 ◽  
pp. 185-187
Author(s):  
S. Orlando ◽  
G. Peres ◽  
S. Serio

AbstractWe have developed a detailed siphon flow model for coronal loops. We find scaling laws relating the characteristic parameters of the loop, explore systematically the space of solutions and show that supersonic flows are impossible for realistic values of heat flux at the base of the upflowing leg.


1993 ◽  
Vol 3 (10) ◽  
pp. 2041-2062 ◽  
Author(s):  
M. J. Thill ◽  
H. J. Hilhorst

2000 ◽  
Vol 627 ◽  
Author(s):  
Prabhu R. Nott ◽  
K. Kesava Rao ◽  
L. Srinivasa Mohan

ABSTRACTThe slow flow of granular materials is often marked by the existence of narrow shear layers, adjacent to large regions that suffer little or no deformation. This behaviour, in the regime where shear stress is generated primarily by the frictional interactions between grains, has so far eluded theoretical description. In this paper, we present a rigid-plastic frictional Cosserat model that captures thin shear layers by incorporating a microscopic length scale. We treat the granular medium as a Cosserat continuum, which allows the existence of localised couple stresses and, therefore, the possibility of an asymmetric stress tensor. In addition, the local rotation is an independent field variable and is not necessarily equal to the vorticity. The angular momentum balance, which is implicitly satisfied for a classical continuum, must now be solved in conjunction with the linear momentum balances. We extend the critical state model, used in soil plasticity, for a Cosserat continuum and obtain predictions for flow in plane and cylindrical Couette devices. The velocity profile predicted by our model is in qualitative agreement with available experimental data. In addition, our model can predict scaling laws for the shear layer thickness as a function of the Couette gap, which must be verified in future experiments. Most significantly, our model can determine the velocity field in viscometric flows, which classical plasticity-based model cannot.


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