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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...

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Detalles Bibliográficos
Autores principales: Mathur, Akshat, Seddighi, Mehdi, He, Shuisheng
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2018
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.
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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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