The anisotropy of the small scale structure in high Reynolds number (Rλ∼1000) turbulent shear flow

被引:188
作者
Shen, X [1 ]
Warhaft, Z [1 ]
机构
[1] Cornell Univ, Ithaca, NY 14853 USA
关键词
D O I
10.1063/1.1313552
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
The postulate of local isotropy (PLI) is tested in a wind tunnel uniform shear flow in which the Reynolds number is varied over the range 100 less than or equal to R(lambda)less than or equal to 1, 100(6.7x10(2)less than or equal to R(l)less than or equal to 6.3x10(4)). The high R-lambda is achieved by using an active grid [Mydlarski and Warhaft, J. Fluid Mech. 320, 331 (1996)] in conjunction with a shear generator. We focus on the increments of the longitudinal velocity fluctuations in the direction of the mean shear. PLI requires that odd order moments of these quantities approach zero as R-lambda-->infinity. Confirming the lower Reynolds number measurements of Garg and Warhaft [Phys. Fluids 10, 662 (1998)], we show that the skewness of partial derivative u/partial derivative y decreases as R-lambda(-0.5) (with a value of 0.2 at R(lambda)similar to 1000). Although the decrease is slower than classical scaling arguments suggest, the result is consistent with PLI, indicating a negligible value at high R-lambda. However, the normalized fifth moment, <(partial derivative u/partial derivative y)(5)>/<(partial derivative u/partial derivative y)(2)>(5/2), is of order 10, and shows no diminution with Reynolds number, while the normalized seventh moment increases with R-lambda. These dissipation range results are inconsistent with PLI. Within the inertial subrange we show that all the odd order moments of the increments of Delta u(y) are nonzero, exhibiting scaling ranges. Here, the skewness structure function has a value similar to 0.5 indicating that in the inertial subrange significant anisotropy is evident even at the third moment level. Fifth- and seventh-order inertial subrange skewness structure functions are of order 10 and 100, respectively. The results show that PLI is untenable, both at dissipation and inertial scales, at least to R(lambda)similar to 1000, and suggest it is unlikely to be so even at higher Reynolds numbers. (C) 2000 American Institute of Physics. [S1070-6631(00)50512-1].
引用
收藏
页码:2976 / 2989
页数:14
相关论文
共 42 条
[1]   ORGANIZED STRUCTURES IN A TURBULENT PLANE JET - TOPOLOGY AND CONTRIBUTION TO MOMENTUM AND HEAT-TRANSPORT [J].
ANTONIA, RA ;
CHAMBERS, AJ ;
BRITZ, D ;
BROWNE, LWB .
JOURNAL OF FLUID MECHANICS, 1986, 172 :211-229
[2]   REYNOLDS-NUMBER DEPENDENCE OF HIGH-ORDER MOMENTS OF THE STREAMWISE TURBULENT VELOCITY DERIVATIVE [J].
ANTONIA, RA ;
CHAMBERS, AJ ;
SATYAPRAKASH, BR .
BOUNDARY-LAYER METEOROLOGY, 1981, 21 (02) :159-171
[3]   EXPERIMENTS ON NEARLY HOMOGENEOUS TURBULENT SHEAR FLOW [J].
CHAMPAGNE, FH ;
HARRIS, VG ;
CORRSIN, S .
JOURNAL OF FLUID MECHANICS, 1970, 41 :81-+
[4]   FINE-SCALE STRUCTURE OF TURBULENT VELOCITY-FIELD [J].
CHAMPAGNE, FH .
JOURNAL OF FLUID MECHANICS, 1978, 86 (MAY) :67-108
[5]   LOCAL ANISOTROPY IN STRAINED TURBULENCE AT HIGH REYNOLDS-NUMBERS [J].
DURBIN, PA ;
SPEZIALE, CG .
JOURNAL OF FLUIDS ENGINEERING-TRANSACTIONS OF THE ASME, 1991, 113 (04) :707-709
[6]   Reynolds number effects on the fine structure of uniformly sheared turbulence [J].
Ferchichi, M ;
Tavoularis, S .
PHYSICS OF FLUIDS, 2000, 12 (11) :2942-2953
[7]  
Frisch U., 1995, TURBULENCE LEGACY AN
[8]   On the small scale structure of simple shear flow [J].
Garg, S ;
Warhaft, Z .
PHYSICS OF FLUIDS, 1998, 10 (03) :662-673
[9]  
GEORGE WK, 1992, EXP FLUIDS, V13, P229, DOI 10.1007/BF00189015
[10]   STRUCTURE OF SHEARED TURBULENT FIELDS [J].
GIBSON, CH ;
FRIEHE, CA ;
MCCONNELL, SO .
PHYSICS OF FLUIDS, 1977, 20 (10) :S156-S167