1994
DOI: 10.1063/1.868214
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Detailed investigation of energy transfers in homogeneous stratified turbulence*

Abstract: This paper investigates some irreversible mechanisms occurring in homogeneous stably stratified turbulent flows. In terms of the eigenmodes of the linear regime, the velocity-temperature field is decomposed into a vortex and two wavy components. Using an eddy-damped quasinormal Markovian (EDQNM) closure with the axisymmetry hypothesis, an analysis of the anisotropic energy transfers between the vortex kinetic energy, the wave kinetic and potential energy is made. Within the light of triadic exchanges, and by a… Show more

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Cited by 126 publications
(133 citation statements)
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“…It is consistent with energy accumulation in the vicinity of k 3 for every energy component and with the results obtained from EDQNM by Godeferd & Cambon [25] ( fig. 1 in their paper) and by Sagaut & Cambon [32] (fig.…”
Section: (B) Energy Anisotropizationsupporting
confidence: 80%
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“…It is consistent with energy accumulation in the vicinity of k 3 for every energy component and with the results obtained from EDQNM by Godeferd & Cambon [25] ( fig. 1 in their paper) and by Sagaut & Cambon [32] (fig.…”
Section: (B) Energy Anisotropizationsupporting
confidence: 80%
“…This tendency corresponds to the formation of a two-component flow as the third, vertical, component collapses. Godeferd & Cambon [25] and Sagaut & Cambon [32] provided a thorough investigation of this behaviour.…”
Section: (B) Energy Anisotropizationmentioning
confidence: 99%
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“…c 1 corresponds to a 'vertical vortex' or toroidal mode, whereas c 2 corresponds to a wave or poloidal mode. Incompressible solutions of equations (12) and (13) in Fourier space and in the Craya-Herring frame are (Godeferd & Cambon, 1994):…”
Section: Linearised Boussinesq Equations With Rotationmentioning
confidence: 99%
“…On the other hand, the numerical treatment of the angular dependence of E (k, t) and Z(k, t) remains a challenge. As an example, the numerical cost of axisymmetric EDQNM models (Godeferd & Cambon 1994;Bellet et al 2006;Favier et al 2011) is much higher than that of the basic EDQNM for isotropic turbulence. These models were developed, from the first case of rotating turbulence (Cambon & Jacquin 1989), for flows dominated by interacting dispersive waves and without explicit linear effect in the governing equation for the energy density E (k, t), requiring the use of the most complicated EDQNM version to handle the effects induced by the mean flow on triple correlations, such as the inhibition of the energy cascade in the case of rotating flows.…”
mentioning
confidence: 99%