On mean flow universality of turbulent wall flows. I. High Reynolds number flow analysis

被引:17
作者
Heinz, Stefan [1 ]
机构
[1] Univ Wyoming, Math Dept, Laramie, WY 82071 USA
基金
美国国家科学基金会;
关键词
Wall-bounded turbulent flows; mean flow structure; universality of wall flows; LARGE-EDDY SIMULATION; DIRECT NUMERICAL-SIMULATION; VELOCITY DISTRIBUTION; BOUNDARY-LAYER; CHANNEL FLOWS; SCALING LAWS; SHEAR FLOWS; PIPE-FLOW; PROFILE; LES;
D O I
10.1080/14685248.2019.1566736
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
The universality and mathematical physical structure of wall-bounded turbulent flows is a topic of discussions over many decades. There is no agreement about questions like what is the physical mean flow structure, how universal is it, and how universal are theoretical concepts for local and global flow variations. These questions are addressed by using latest direct numerical simulation (DNS) data at moderate Reynolds numbers Re and experimental data up to extreme Re. The mean flow structure is explained by analytical models for three canonical wall-bounded turbulent flows (channel flow, pipe flow, and the zero-pressure gradient turbulent boundary layer). Thorough comparisons with DNS and experimental data provide support for the validity of models. Criteria for veritable physics derived from observations are suggested. It is shown that the models presented satisfy these criteria. A probabilistic interpretation of the mean flow structure shows that the physical constraints of equal entropies and equally likely mean velocity values in a region unaffected by boundary effects impose a universal log-law structure. The structure of wall-bounded turbulent flows is much more universal than previously expected. There is no discrepancy between local logarithmic velocity variations and global friction law and bulk velocity variations. Flow effects are limited to the minimum: the difference of having a bounded or unbounded domain, and the variation range of mean velocity values allowed by the geometry.
引用
收藏
页码:929 / 958
页数:30
相关论文
共 99 条
[71]   The interaction between inner and outer regions of turbulent wall-bounded flow [J].
Morrison, Jonathan F. .
PHILOSOPHICAL TRANSACTIONS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 2007, 365 (1852) :683-698
[72]   EXPLICIT EXPRESSION FOR THE SMOOTH WALL VELOCITY DISTRIBUTION IN A TURBULENT BOUNDARY-LAYER [J].
MUSKER, AJ .
AIAA JOURNAL, 1979, 17 (06) :655-657
[73]   Comparison of turbulent channel and pipe flows with varying Reynolds number [J].
Ng, H. C. H. ;
Monty, J. P. ;
Hutchins, N. ;
Chong, M. S. ;
Marusic, I. .
EXPERIMENTS IN FLUIDS, 2011, 51 (05) :1261-1281
[74]   Inner scaling for wall-bounded flows subject to large pressure gradients [J].
Nickels, TB .
JOURNAL OF FLUID MECHANICS, 2004, 521 :217-239
[75]   A unified approach for symmetries in plane parallel turbulent shear flows [J].
Oberlack, M .
JOURNAL OF FLUID MECHANICS, 2001, 427 :299-328
[76]   LES approach for high Reynolds number wall-bounded flows with application to turbulent channel flow [J].
Pantano, C. ;
Pullin, D. I. ;
Dimotakis, P. E. ;
Matheou, G. .
JOURNAL OF COMPUTATIONAL PHYSICS, 2008, 227 (21) :9271-9291
[77]   Composite asymptotic expansions and scaling wall turbulence [J].
Panton, Ronald L. .
PHILOSOPHICAL TRANSACTIONS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 2007, 365 (1852) :733-754
[78]  
Pope SB., 2000, TURBULENT FLOWS, DOI [DOI 10.1017/CBO9780511840531, 10.1017/CBO9780511840531]
[79]   On the asymptotic state of high Reynolds number, smooth-wall turbulent flows [J].
Pullin, D. I. ;
Inoue, M. ;
Saito, N. .
PHYSICS OF FLUIDS, 2013, 25 (01)
[80]  
Reichardt H., 1951, ZAMM J. Appl. Math. Mech./Z. Angew. Math. Mech, V31, P208, DOI [10.1002/zamm.19510310704, DOI 10.1002/ZAMM.19510310704]