A LOW-SHEAR TURBULENT BOUNDARY-LAYER

Citation
J. Hamelin et Ae. Alving, A LOW-SHEAR TURBULENT BOUNDARY-LAYER, Physics of fluids, 8(3), 1996, pp. 789-804
Citations number
23
Categorie Soggetti
Mechanics,"Phsycs, Fluid & Plasmas
Journal title
ISSN journal
10706631
Volume
8
Issue
3
Year of publication
1996
Pages
789 - 804
Database
ISI
SICI code
1070-6631(1996)8:3<789:ALTB>2.0.ZU;2-4
Abstract
This paper describes experimental results measured in a low-shear turb ulent boundary layer. The low-shear condition is exerted after the bou ndary layer reaches Re(theta)similar or equal to 2000 and has the effe ct of removing the inner layer; thus, these are the first results to s how the behavior of an outer-layer-only turbulent boundary layer. The removal of the inner layer causes the gradual decay of the turbulent s tresses over eleven boundary-layer thicknesses (roughly 20 large-eddy length scales) of streamwise distance, with the decay beginning at the wall and propagating into the outer flow with increasing downstream d istance. However, the structure of the outer layer is little affected by the perturbation, as demonstrated by stress (anisotropy) ratios, qu adrant analysis, and spectral measurements. Although the lack of near- wall production implies this flow must eventually decay into isotropic turbulence, this decay occurs relatively slowly because the dissipati on is also greatly reduced with the decrease in near-wall shear. In ad dition, the outer-layer production is significant in maintaining the t urbulence level. These results show that, once formed, the outer-layer characteristics are not explicitly dependent on the presence of the i nner layer. These results are compared with similar studies of isotrop ic turbulence near a shear-free wall. Very close to the wall the two f lows both show that the normal-stress components respond differently t o the presence of the wall. However, away from the wall the isotropic results underpredict the distance to which the tangential stresses are damped by the impermeability condition at the wall. Finally, the resu lts show general similarities to those in a boundary layer just downst ream of reattachment, after a similar low-shear condition over the sep aration bubble. This raises the possibility that many of the important features of the reattaching flow can be captured by the present, simp ler experiment. (C) 1996 American Institute of Physics.