Decay of Batchelor and Saffman rotating turbulence

The decay rate of isotropic and homogeneous turbulence is known to be affected by the large-scale spectrum of the initial perturbations, associated with at least two canonical self-preserving solutions of the von Kármán-Howarth equation: the so-called Batchelor and Saffman spectra. The effect of lon...

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Autores principales: Teitelbaum, Tomás, Mininni, Pablo Daniel
Publicado: 2012
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Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15393755_v86_n6_p_Teitelbaum
http://hdl.handle.net/20.500.12110/paper_15393755_v86_n6_p_Teitelbaum
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spelling paper:paper_15393755_v86_n6_p_Teitelbaum2023-06-08T16:20:55Z Decay of Batchelor and Saffman rotating turbulence Teitelbaum, Tomás Mininni, Pablo Daniel Anisotropic flows Decay rate Flow evolution Homogeneous turbulence Initial energy Initial perturbation Integral quantity Long range correlations Power-law Rotating turbulence Self-similar Total energy Anisotropy Decay (organic) The decay rate of isotropic and homogeneous turbulence is known to be affected by the large-scale spectrum of the initial perturbations, associated with at least two canonical self-preserving solutions of the von Kármán-Howarth equation: the so-called Batchelor and Saffman spectra. The effect of long-range correlations in the decay of anisotropic flows is less clear, and recently it has been proposed that the decay rate of rotating turbulence may be independent of the large-scale spectrum of the initial perturbations. We analyze numerical simulations of freely decaying rotating turbulence with initial energy spectra ∼k4 (Batchelor turbulence) and ∼k2 (Saffman turbulence) and show that, while a self-similar decay can not be identified for the total energy, the decay is indeed affected by long-range correlations. The decay of two- and three-dimensional modes follows distinct power laws in each case, which are consistent with predictions derived from the anisotropic von Kármán-Howarth equation, and with conservation of anisotropic integral quantities by the flow evolution. © 2012 American Physical Society. Fil:Teitelbaum, T. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Mininni, P.D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 2012 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15393755_v86_n6_p_Teitelbaum http://hdl.handle.net/20.500.12110/paper_15393755_v86_n6_p_Teitelbaum
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Anisotropic flows
Decay rate
Flow evolution
Homogeneous turbulence
Initial energy
Initial perturbation
Integral quantity
Long range correlations
Power-law
Rotating turbulence
Self-similar
Total energy
Anisotropy
Decay (organic)
spellingShingle Anisotropic flows
Decay rate
Flow evolution
Homogeneous turbulence
Initial energy
Initial perturbation
Integral quantity
Long range correlations
Power-law
Rotating turbulence
Self-similar
Total energy
Anisotropy
Decay (organic)
Teitelbaum, Tomás
Mininni, Pablo Daniel
Decay of Batchelor and Saffman rotating turbulence
topic_facet Anisotropic flows
Decay rate
Flow evolution
Homogeneous turbulence
Initial energy
Initial perturbation
Integral quantity
Long range correlations
Power-law
Rotating turbulence
Self-similar
Total energy
Anisotropy
Decay (organic)
description The decay rate of isotropic and homogeneous turbulence is known to be affected by the large-scale spectrum of the initial perturbations, associated with at least two canonical self-preserving solutions of the von Kármán-Howarth equation: the so-called Batchelor and Saffman spectra. The effect of long-range correlations in the decay of anisotropic flows is less clear, and recently it has been proposed that the decay rate of rotating turbulence may be independent of the large-scale spectrum of the initial perturbations. We analyze numerical simulations of freely decaying rotating turbulence with initial energy spectra ∼k4 (Batchelor turbulence) and ∼k2 (Saffman turbulence) and show that, while a self-similar decay can not be identified for the total energy, the decay is indeed affected by long-range correlations. The decay of two- and three-dimensional modes follows distinct power laws in each case, which are consistent with predictions derived from the anisotropic von Kármán-Howarth equation, and with conservation of anisotropic integral quantities by the flow evolution. © 2012 American Physical Society.
author Teitelbaum, Tomás
Mininni, Pablo Daniel
author_facet Teitelbaum, Tomás
Mininni, Pablo Daniel
author_sort Teitelbaum, Tomás
title Decay of Batchelor and Saffman rotating turbulence
title_short Decay of Batchelor and Saffman rotating turbulence
title_full Decay of Batchelor and Saffman rotating turbulence
title_fullStr Decay of Batchelor and Saffman rotating turbulence
title_full_unstemmed Decay of Batchelor and Saffman rotating turbulence
title_sort decay of batchelor and saffman rotating turbulence
publishDate 2012
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_15393755_v86_n6_p_Teitelbaum
http://hdl.handle.net/20.500.12110/paper_15393755_v86_n6_p_Teitelbaum
work_keys_str_mv AT teitelbaumtomas decayofbatchelorandsaffmanrotatingturbulence
AT mininnipablodaniel decayofbatchelorandsaffmanrotatingturbulence
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