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Transition of Transient Channel Flow with High Reynolds Number Ratios
Large-eddy simulations of turbulent channel flow subjected to a step-like acceleration have been performed to investigate the effect of high Reynolds number ratios on the transient behaviour of turbulence. It is shown that the response of the flow exhibits the same fundamental characteristics descri...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7512894/ https://www.ncbi.nlm.nih.gov/pubmed/33265465 http://dx.doi.org/10.3390/e20050375 |
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author | Mathur, Akshat Seddighi, Mehdi He, Shuisheng |
author_facet | Mathur, Akshat Seddighi, Mehdi He, Shuisheng |
author_sort | Mathur, Akshat |
collection | PubMed |
description | Large-eddy simulations of turbulent channel flow subjected to a step-like acceleration have been performed to investigate the effect of high Reynolds number ratios on the transient behaviour of turbulence. It is shown that the response of the flow exhibits the same fundamental characteristics described in He & Seddighi (J. Fluid Mech., vol. 715, 2013, pp. 60–102 and vol. 764, 2015, pp. 395–427)—a three-stage response resembling that of the bypass transition of boundary layer flows. The features of transition are seen to become more striking as the Re-ratio increases—the elongated streaks become stronger and longer, and the initial turbulent spot sites at the onset of transition become increasingly sparse. The critical Reynolds number of transition and the transition period Reynolds number for those cases are shown to deviate from the trends of He & Seddighi (2015). The high Re-ratio cases show double peaks in the transient response of streamwise fluctuation profiles shortly after the onset of transition. Conditionally-averaged turbulent statistics based on a λ_2-criterion are used to show that the two peaks in the fluctuation profiles are due to separate contributions of the active and inactive regions of turbulence generation. The peak closer to the wall is attributed to the generation of “new” turbulence in the active region, whereas the peak farther away from the wall is attributed to the elongated streaks in the inactive region. In the low Re-ratio cases, the peaks of these two regions are close to each other during the entire transient, resulting in a single peak in the domain-averaged profile. |
format | Online Article Text |
id | pubmed-7512894 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-75128942020-11-09 Transition of Transient Channel Flow with High Reynolds Number Ratios Mathur, Akshat Seddighi, Mehdi He, Shuisheng Entropy (Basel) Article Large-eddy simulations of turbulent channel flow subjected to a step-like acceleration have been performed to investigate the effect of high Reynolds number ratios on the transient behaviour of turbulence. It is shown that the response of the flow exhibits the same fundamental characteristics described in He & Seddighi (J. Fluid Mech., vol. 715, 2013, pp. 60–102 and vol. 764, 2015, pp. 395–427)—a three-stage response resembling that of the bypass transition of boundary layer flows. The features of transition are seen to become more striking as the Re-ratio increases—the elongated streaks become stronger and longer, and the initial turbulent spot sites at the onset of transition become increasingly sparse. The critical Reynolds number of transition and the transition period Reynolds number for those cases are shown to deviate from the trends of He & Seddighi (2015). The high Re-ratio cases show double peaks in the transient response of streamwise fluctuation profiles shortly after the onset of transition. Conditionally-averaged turbulent statistics based on a λ_2-criterion are used to show that the two peaks in the fluctuation profiles are due to separate contributions of the active and inactive regions of turbulence generation. The peak closer to the wall is attributed to the generation of “new” turbulence in the active region, whereas the peak farther away from the wall is attributed to the elongated streaks in the inactive region. In the low Re-ratio cases, the peaks of these two regions are close to each other during the entire transient, resulting in a single peak in the domain-averaged profile. MDPI 2018-05-17 /pmc/articles/PMC7512894/ /pubmed/33265465 http://dx.doi.org/10.3390/e20050375 Text en © 2018 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Mathur, Akshat Seddighi, Mehdi He, Shuisheng Transition of Transient Channel Flow with High Reynolds Number Ratios |
title | Transition of Transient Channel Flow with High Reynolds Number Ratios |
title_full | Transition of Transient Channel Flow with High Reynolds Number Ratios |
title_fullStr | Transition of Transient Channel Flow with High Reynolds Number Ratios |
title_full_unstemmed | Transition of Transient Channel Flow with High Reynolds Number Ratios |
title_short | Transition of Transient Channel Flow with High Reynolds Number Ratios |
title_sort | transition of transient channel flow with high reynolds number ratios |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7512894/ https://www.ncbi.nlm.nih.gov/pubmed/33265465 http://dx.doi.org/10.3390/e20050375 |
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