1107 Similarity of the Reynolds Stress Profiles for Outer-layer in Turbulent Boundary Layers(1)

2006 ◽  
Vol 2006 (0) ◽  
pp. _1107-a_
Author(s):  
Takatsugu KAMEDA ◽  
Shinsuke MOCHIZUKI ◽  
Hideo OSAKA
AIAA Journal ◽  
1989 ◽  
Vol 27 (1) ◽  
pp. 15-22 ◽  
Author(s):  
Richard A. Wahls ◽  
Richard W. Barnwell ◽  
Fred R. DeJarnette

1973 ◽  
Vol 60 (1) ◽  
pp. 43-62 ◽  
Author(s):  
Ronald M. C. So ◽  
George L. Mellor

Turbulent boundary layers along a convex surface of varying curvature were investigated in a specially designed boundary-layer tunnel. A fairly complete set of turbulence measurements was obtained.The effect of curvature is striking. For example, along a convex wall the Reynolds stress is decreased near the wall and vanishes about midway between the wall and the edge of a boundary layer where there exists a velocity profile gradient created upstream of the curved wall.


1996 ◽  
Vol 118 (4) ◽  
pp. 787-794 ◽  
Author(s):  
A. C. Schwarz ◽  
M. W. Plesniak

A turbulent boundary layer subjected to multiple, additional strain rates, namely convex curvature coupled with streamwise pressure gradients (zero and favorable, ZPG and FPG) was investigated experimentally using laser Doppler velocimetry. The inapplicability of the universal flat-plate log-law to curved flows is discussed. However, a logarithmic region is found in the curved and accelerated turbulent boundary layer examined here. Similarity of the mean velocity and Reynolds stress profiles was achieved by 45 deg of curvature even in the presence of the strongest FPG investigated (k = 1.01 × 10−6). The Reynolds stresses were suppressed (with respect to flat plate values) due primarily to the effects of strong convex curvature (δo/R ≈ 0.10). In curved boundary layers subjected to different favorable pressure gradients, the mean velocity and normal Reynolds stress profiles collapsed in the inner region, but deviated in the outer region (y+ ≥ 100). Thus, inner scaling accounted for the impact of the extra strain rates on these profiles in the near-wall region. Combined with curvature, the FPG reduced the strength of the wake component, resulted in a greater suppression of the fluctuating velocity components and a reduction of the primary Reynolds shear stress throughout almost the entire boundary layer relative to the ZPG curved case.


1988 ◽  
Vol 31 (10) ◽  
pp. 2814 ◽  
Author(s):  
Alexander Sahlin ◽  
Arne V. Johansson ◽  
P. Henrik Alfredsson

2005 ◽  
Vol 38 (3) ◽  
pp. 328-340 ◽  
Author(s):  
M. P. Schultz ◽  
K. A. Flack

Sign in / Sign up

Export Citation Format

Share Document