Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence

Rapidly rotating turbulent flow is characterized by the emergence of columnar structures that are representative of quasi-two-dimensional behavior of the flow. It is known that when energy is injected into the fluid at an intermediate scale L f, it cascades towards smaller as well as larger scales....

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Autores principales: Sen, A., Mininni, P.D., Rosenberg, D., Pouquet, A.
Formato: Artículo publishedVersion
Lenguaje:Inglés
Publicado: 2012
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_15393755_v86_n3_p_Sen
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spelling paperaa:paper_15393755_v86_n3_p_Sen2023-06-12T16:50:42Z Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence Phys. Rev. E Stat. Nonlinear Soft Matter Phys. 2012;86(3) Sen, A. Mininni, P.D. Rosenberg, D. Pouquet, A. Columnar structures Eddy viscosity Forcing function Forcings Helicities Large-scale energy spectrum Nonuniversality Per unit Quasi-two-dimensional behavior Rossby numbers Rotating turbulence Small scale Time-scales Total energy Two-dimensional (2D) turbulence Wave numbers Anisotropy Aspect ratio Reynolds number Spectroscopy Three dimensional computer graphics Shear flow Rapidly rotating turbulent flow is characterized by the emergence of columnar structures that are representative of quasi-two-dimensional behavior of the flow. It is known that when energy is injected into the fluid at an intermediate scale L f, it cascades towards smaller as well as larger scales. In this paper we analyze the flow in the inverse cascade range at a small but fixed Rossby number, Ro f≈0.05. Several numerical simulations with helical and nonhelical forcing functions are considered in periodic boxes with unit aspect ratio. In order to resolve the inverse cascade range with reasonably large Reynolds number, the analysis is based on large eddy simulations which include the effect of helicity on eddy viscosity and eddy noise. Thus, we model the small scales and resolve explicitly the large scales. We show that the large-scale energy spectrum has at least two solutions: one that is consistent with Kolmogorov-Kraichnan-Batchelor-Leith phenomenology for the inverse cascade of energy in two-dimensional (2D) turbulence with a ∼k⊥-5/3 scaling, and the other that corresponds to a steeper ∼k⊥-3 spectrum in which the three-dimensional (3D) modes release a substantial fraction of their energy per unit time to the 2D modes. The spectrum that emerges depends on the anisotropy of the forcing function, the former solution prevailing for forcings in which more energy is injected into the 2D modes while the latter prevails for isotropic forcing. In the case of anisotropic forcing, whence the energy goes from the 2D to the 3D modes at low wave numbers, large-scale shear is created, resulting in a time scale τ sh, associated with shear, thereby producing a ∼k -1 spectrum for the total energy with the horizontal energy of the 2D modes still following a ∼k⊥-5/3 scaling. © 2012 American Physical Society. Fil:Mininni, P.D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. 2012 info:eu-repo/semantics/article info:ar-repo/semantics/artículo info:eu-repo/semantics/publishedVersion application/pdf eng info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_15393755_v86_n3_p_Sen
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
language Inglés
orig_language_str_mv eng
topic Columnar structures
Eddy viscosity
Forcing function
Forcings
Helicities
Large-scale energy spectrum
Nonuniversality
Per unit
Quasi-two-dimensional behavior
Rossby numbers
Rotating turbulence
Small scale
Time-scales
Total energy
Two-dimensional (2D) turbulence
Wave numbers
Anisotropy
Aspect ratio
Reynolds number
Spectroscopy
Three dimensional computer graphics
Shear flow
spellingShingle Columnar structures
Eddy viscosity
Forcing function
Forcings
Helicities
Large-scale energy spectrum
Nonuniversality
Per unit
Quasi-two-dimensional behavior
Rossby numbers
Rotating turbulence
Small scale
Time-scales
Total energy
Two-dimensional (2D) turbulence
Wave numbers
Anisotropy
Aspect ratio
Reynolds number
Spectroscopy
Three dimensional computer graphics
Shear flow
Sen, A.
Mininni, P.D.
Rosenberg, D.
Pouquet, A.
Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
topic_facet Columnar structures
Eddy viscosity
Forcing function
Forcings
Helicities
Large-scale energy spectrum
Nonuniversality
Per unit
Quasi-two-dimensional behavior
Rossby numbers
Rotating turbulence
Small scale
Time-scales
Total energy
Two-dimensional (2D) turbulence
Wave numbers
Anisotropy
Aspect ratio
Reynolds number
Spectroscopy
Three dimensional computer graphics
Shear flow
description Rapidly rotating turbulent flow is characterized by the emergence of columnar structures that are representative of quasi-two-dimensional behavior of the flow. It is known that when energy is injected into the fluid at an intermediate scale L f, it cascades towards smaller as well as larger scales. In this paper we analyze the flow in the inverse cascade range at a small but fixed Rossby number, Ro f≈0.05. Several numerical simulations with helical and nonhelical forcing functions are considered in periodic boxes with unit aspect ratio. In order to resolve the inverse cascade range with reasonably large Reynolds number, the analysis is based on large eddy simulations which include the effect of helicity on eddy viscosity and eddy noise. Thus, we model the small scales and resolve explicitly the large scales. We show that the large-scale energy spectrum has at least two solutions: one that is consistent with Kolmogorov-Kraichnan-Batchelor-Leith phenomenology for the inverse cascade of energy in two-dimensional (2D) turbulence with a ∼k⊥-5/3 scaling, and the other that corresponds to a steeper ∼k⊥-3 spectrum in which the three-dimensional (3D) modes release a substantial fraction of their energy per unit time to the 2D modes. The spectrum that emerges depends on the anisotropy of the forcing function, the former solution prevailing for forcings in which more energy is injected into the 2D modes while the latter prevails for isotropic forcing. In the case of anisotropic forcing, whence the energy goes from the 2D to the 3D modes at low wave numbers, large-scale shear is created, resulting in a time scale τ sh, associated with shear, thereby producing a ∼k -1 spectrum for the total energy with the horizontal energy of the 2D modes still following a ∼k⊥-5/3 scaling. © 2012 American Physical Society.
format Artículo
Artículo
publishedVersion
author Sen, A.
Mininni, P.D.
Rosenberg, D.
Pouquet, A.
author_facet Sen, A.
Mininni, P.D.
Rosenberg, D.
Pouquet, A.
author_sort Sen, A.
title Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
title_short Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
title_full Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
title_fullStr Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
title_full_unstemmed Anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
title_sort anisotropy and nonuniversality in scaling laws of the large-scale energy spectrum in rotating turbulence
publishDate 2012
url http://hdl.handle.net/20.500.12110/paper_15393755_v86_n3_p_Sen
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AT rosenbergd anisotropyandnonuniversalityinscalinglawsofthelargescaleenergyspectruminrotatingturbulence
AT pouqueta anisotropyandnonuniversalityinscalinglawsofthelargescaleenergyspectruminrotatingturbulence
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