Direct numerical simulation of turbulence over two-dimensional waves
Knowledge of turbulent flows over non-flat surfaces is of major practical interest in diverse applications. Significant work continues to be reported in the roughness regime at high Reynolds numbers where the cumulative effect of surface undulations on the averaged and integrated turbulence quantiti...
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Online Access: | http://dx.doi.org/10.1063/1.5140000 |
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doaj-880f82f6c43a4290851334bdc7912adb2020-11-25T01:45:06ZengAIP Publishing LLCAIP Advances2158-32262020-02-01102025034025034-2510.1063/1.5140000Direct numerical simulation of turbulence over two-dimensional wavesBalaji Jayaraman0Saadbin Khan1School of Mechanical and Aerospace Engineering, Oklahoma State University, Stillwater, Oklahoma 74078, USASchool of Mechanical and Aerospace Engineering, Oklahoma State University, Stillwater, Oklahoma 74078, USAKnowledge of turbulent flows over non-flat surfaces is of major practical interest in diverse applications. Significant work continues to be reported in the roughness regime at high Reynolds numbers where the cumulative effect of surface undulations on the averaged and integrated turbulence quantities is well documented. Even for such cases, the surface topology plays an important role for transitional roughness Reynolds numbers that is hard to characterize. In this work, we explore in detail the mechanisms underlying turbulence generation and transport, particularly within the region of the turbulent boundary layer affected by the surface. We relate surface shape with turbulence generation mechanisms and Reynolds stress transport, which has implications to drag increase. We accomplish this using a suite of direct numerical simulations of fully developed turbulent flow between two infinitely wide, two-dimensional sinusoidally wavy surfaces at a friction Reynolds number, Reτ = 180, with different mean surface slopes, ζ (and fixed inner-scaled undulation height, a+ = 13), corresponding to the “waviness” regime. The increase in wave slope enhances near surface turbulent mixing, resulting in increased total drag, higher fraction of form drag, faster approach to isotropy, and thereby modulation of the buffer layer. The primary near-surface streamwise and vertical turbulence production occurs in the leeward and windward sides of the wave, respectively. Furthermore, this production structure shows significant dispersion effects. However, the primary generation process of vertical and spanwise variance occurs through pressure–strain rate mechanism in the windward side.http://dx.doi.org/10.1063/1.5140000 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Balaji Jayaraman Saadbin Khan |
spellingShingle |
Balaji Jayaraman Saadbin Khan Direct numerical simulation of turbulence over two-dimensional waves AIP Advances |
author_facet |
Balaji Jayaraman Saadbin Khan |
author_sort |
Balaji Jayaraman |
title |
Direct numerical simulation of turbulence over two-dimensional waves |
title_short |
Direct numerical simulation of turbulence over two-dimensional waves |
title_full |
Direct numerical simulation of turbulence over two-dimensional waves |
title_fullStr |
Direct numerical simulation of turbulence over two-dimensional waves |
title_full_unstemmed |
Direct numerical simulation of turbulence over two-dimensional waves |
title_sort |
direct numerical simulation of turbulence over two-dimensional waves |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2020-02-01 |
description |
Knowledge of turbulent flows over non-flat surfaces is of major practical interest in diverse applications. Significant work continues to be reported in the roughness regime at high Reynolds numbers where the cumulative effect of surface undulations on the averaged and integrated turbulence quantities is well documented. Even for such cases, the surface topology plays an important role for transitional roughness Reynolds numbers that is hard to characterize. In this work, we explore in detail the mechanisms underlying turbulence generation and transport, particularly within the region of the turbulent boundary layer affected by the surface. We relate surface shape with turbulence generation mechanisms and Reynolds stress transport, which has implications to drag increase. We accomplish this using a suite of direct numerical simulations of fully developed turbulent flow between two infinitely wide, two-dimensional sinusoidally wavy surfaces at a friction Reynolds number, Reτ = 180, with different mean surface slopes, ζ (and fixed inner-scaled undulation height, a+ = 13), corresponding to the “waviness” regime. The increase in wave slope enhances near surface turbulent mixing, resulting in increased total drag, higher fraction of form drag, faster approach to isotropy, and thereby modulation of the buffer layer. The primary near-surface streamwise and vertical turbulence production occurs in the leeward and windward sides of the wave, respectively. Furthermore, this production structure shows significant dispersion effects. However, the primary generation process of vertical and spanwise variance occurs through pressure–strain rate mechanism in the windward side. |
url |
http://dx.doi.org/10.1063/1.5140000 |
work_keys_str_mv |
AT balajijayaraman directnumericalsimulationofturbulenceovertwodimensionalwaves AT saadbinkhan directnumericalsimulationofturbulenceovertwodimensionalwaves |
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