Inverse cascades in turbulence and the case of rotating flows

We first summarize briefly several properties concerning the dynamics of two-dimensional (2D) turbulence, with an emphasis on the inverse cascade of energy to the largest accessible scale of the system. In order to study a similar phenomenon in 3D turbulence undergoing strong solid-body rotation, we...

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Autores principales: Pouquet, A., Sen, A., Rosenberg, D., Mininni, P.D., Baerenzung, J.
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_00318949_v88_nT155_p_Pouquet
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spelling todo:paper_00318949_v88_nT155_p_Pouquet2023-10-03T14:41:51Z Inverse cascades in turbulence and the case of rotating flows Pouquet, A. Sen, A. Rosenberg, D. Mininni, P.D. Baerenzung, J. Energy spectra High resolution Inverse energy cascades Numerical results Rotating flow Rotating turbulence Solid-body rotation Two-dimensional (2D) turbulence Large eddy simulation Rotational flow Shear flow Turbulence Mixing Shock tubes Turbulent flow Three dimensional We first summarize briefly several properties concerning the dynamics of two-dimensional (2D) turbulence, with an emphasis on the inverse cascade of energy to the largest accessible scale of the system. In order to study a similar phenomenon in 3D turbulence undergoing strong solid-body rotation, we test a previously developed large eddy simulation (LES) model against a high-resolution direct numerical simulation of rotating turbulence on a grid of 30723 points. We then describe new numerical results on the inverse energy cascade in rotating flows using this LES model and contrast the case of 2D versus 3D forcing, as well as non-helical forcing (i.e. with weak overall alignment between velocity and vorticity) versus the fully helical Beltrami case, for both deterministic and random forcing. The different scaling laws for the inverse energy cascade can be attributed to the dimensionality of the forcing, with either a k-3⊥ or a k -5/3⊥ energy spectrum of slow modes at large scales, k⊥ referring to a direction perpendicular to that of rotation. We finally invoke the role of shear in the case of a strongly anisotropic deterministic forcing, using the so-called ABC flow; in that case, a k -5/3⊥ is again observed for the slow modes, together with a k-1 spectrum for the total energy associated with enhanced shear at a large scale [92]. © 2013 The Royal Swedish Academy of Sciences. Fil:Mininni, P.D. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_00318949_v88_nT155_p_Pouquet
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Energy spectra
High resolution
Inverse energy cascades
Numerical results
Rotating flow
Rotating turbulence
Solid-body rotation
Two-dimensional (2D) turbulence
Large eddy simulation
Rotational flow
Shear flow
Turbulence
Mixing
Shock tubes
Turbulent flow
Three dimensional
spellingShingle Energy spectra
High resolution
Inverse energy cascades
Numerical results
Rotating flow
Rotating turbulence
Solid-body rotation
Two-dimensional (2D) turbulence
Large eddy simulation
Rotational flow
Shear flow
Turbulence
Mixing
Shock tubes
Turbulent flow
Three dimensional
Pouquet, A.
Sen, A.
Rosenberg, D.
Mininni, P.D.
Baerenzung, J.
Inverse cascades in turbulence and the case of rotating flows
topic_facet Energy spectra
High resolution
Inverse energy cascades
Numerical results
Rotating flow
Rotating turbulence
Solid-body rotation
Two-dimensional (2D) turbulence
Large eddy simulation
Rotational flow
Shear flow
Turbulence
Mixing
Shock tubes
Turbulent flow
Three dimensional
description We first summarize briefly several properties concerning the dynamics of two-dimensional (2D) turbulence, with an emphasis on the inverse cascade of energy to the largest accessible scale of the system. In order to study a similar phenomenon in 3D turbulence undergoing strong solid-body rotation, we test a previously developed large eddy simulation (LES) model against a high-resolution direct numerical simulation of rotating turbulence on a grid of 30723 points. We then describe new numerical results on the inverse energy cascade in rotating flows using this LES model and contrast the case of 2D versus 3D forcing, as well as non-helical forcing (i.e. with weak overall alignment between velocity and vorticity) versus the fully helical Beltrami case, for both deterministic and random forcing. The different scaling laws for the inverse energy cascade can be attributed to the dimensionality of the forcing, with either a k-3⊥ or a k -5/3⊥ energy spectrum of slow modes at large scales, k⊥ referring to a direction perpendicular to that of rotation. We finally invoke the role of shear in the case of a strongly anisotropic deterministic forcing, using the so-called ABC flow; in that case, a k -5/3⊥ is again observed for the slow modes, together with a k-1 spectrum for the total energy associated with enhanced shear at a large scale [92]. © 2013 The Royal Swedish Academy of Sciences.
format JOUR
author Pouquet, A.
Sen, A.
Rosenberg, D.
Mininni, P.D.
Baerenzung, J.
author_facet Pouquet, A.
Sen, A.
Rosenberg, D.
Mininni, P.D.
Baerenzung, J.
author_sort Pouquet, A.
title Inverse cascades in turbulence and the case of rotating flows
title_short Inverse cascades in turbulence and the case of rotating flows
title_full Inverse cascades in turbulence and the case of rotating flows
title_fullStr Inverse cascades in turbulence and the case of rotating flows
title_full_unstemmed Inverse cascades in turbulence and the case of rotating flows
title_sort inverse cascades in turbulence and the case of rotating flows
url http://hdl.handle.net/20.500.12110/paper_00318949_v88_nT155_p_Pouquet
work_keys_str_mv AT pouqueta inversecascadesinturbulenceandthecaseofrotatingflows
AT sena inversecascadesinturbulenceandthecaseofrotatingflows
AT rosenbergd inversecascadesinturbulenceandthecaseofrotatingflows
AT mininnipd inversecascadesinturbulenceandthecaseofrotatingflows
AT baerenzungj inversecascadesinturbulenceandthecaseofrotatingflows
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