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2005b On the double cascades of energy and enstrophy in two dimensional turbulence. Part 2. Approach to the KLB limit and interpretation of experimental evidence. Discrete Contin (0)

by E Gkioulekas, K Tung
Venue:Dyn. Syst. Ser. B
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Multiresolution analysis for 2D turbulence. Part 2: A physical interpretation

by Ch. -h. Bruneau, P. Fischer, H. Kellay - Discrete and Continuous Dynamical Systems B 2007
"... Abstract. Multiresolution methods like the wavelet packets or the cosine packets are more and more used in physical applications and in particular in two-dimensional turbulence. The theoretical bases of these decompositions have been introduced in the first part of this paper. The numerical results ..."
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Abstract. Multiresolution methods like the wavelet packets or the cosine packets are more and more used in physical applications and in particular in two-dimensional turbulence. The theoretical bases of these decompositions have been introduced in the first part of this paper. The numerical results have shown that the wavelet packets decomposition is well suited for studying this kind of problem: the visualization of the vorticity field is better, without any kind of artifacts contrary to the visualization with the cosine packets filtering. The current second part of the paper is devoted to the physical interpretation of the filtering process proposed in the first part. Only the wavelet packets decomposition is considered here since the cosine packets did not give an entire satisfaction. 1. Introduction. We have shown in the first part of this paper [6] that the wavelet packets filtering can be successfully used for analyzing two-dimensional turbulence. This technique allows to separate two kinds of structures, the solid rotations com-posed by the core of the vortices from the background mainly composed by vorticity
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...eading cascades, upscales for the inverse energy cascade and downscales for the direct enstrophy cascade but also the existence of subleading cascades as theoretically shown by Tung and Gkioulekas in =-=[9, 10]-=- and [16]. It can also be noticed that the injection scale being relatively large, the energy cascade cannot be developed completely. On the other side, the enstrophy cascade does not present any “pla...

Is the subdominant part of the energy spectrum due to downscale energy cascade hidden in quasi-geostrophic turbulence?

by Eleftherios Gkioulekas, Ka Kit Tung , 2006
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...safely ignored. Predicting the form of these subleading corrections requires a subtle mathematical argument that goes beyond dimensional analysis. Such an argument was given previously by the authors =-=[25, 26]-=- as follows: the subleading fluxes are associated with a subleading downscale energy cascade and a subleading inverse enstrophy cascade that contribute linearly to the total energy spectrum in additio...

Recent developments in understanding two-dimensional turbulence and the Nastrom-Gage spectrum

by Eleftherios Gkioulekas, Ka-kit Tung , 608
"... Two-dimensional turbulence appears to be a more formidable problem than three-dimensional turbulence despite the numerical advantage of working with one less dimension. In the present paper we review recent numerical investigations of the phenomenology of two-dimensional turbulence as well as recent ..."
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Two-dimensional turbulence appears to be a more formidable problem than three-dimensional turbulence despite the numerical advantage of working with one less dimension. In the present paper we review recent numerical investigations of the phenomenology of two-dimensional turbulence as well as recent theoretical breakthroughs by various leading researchers. We also review efforts to reconcile the observed energy spectrum of the atmosphere (the spectrum) with the predictions of two-dimensional turbulence and quasigeostrophic turbulence. PACS numbers: 42.68.Bz, 47.27.-i, 47.27.ek, 92.60.hk, 92.10.ak 1.
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...clude momentum dissipation of relative vorticity, in each 23layer, and Ekman damping from the lower boundary layer, and they read: d1 = (−1) κ+1 ν∇ 2κ ζ1 (51) d2 = (−1) κ+1 ν∇ 2κ ζ2 (52) e2 = −νEζ2. =-=(53)-=- This model can be reduced to a coupled 2D-like system by employing the temperature equation to eliminate the vertical velocity ω. This leads to the definition of the potential vorticity q1 and q2 as ...

A theoretical study of the cascades of 3D, 2D, and QG turbulence

by Eleftherios Gkioulekas , 2006
"... ..."
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Remarks on the Frisch framework of hydrodynamic turbulence and the quasi-Lagrangian formulation

by Eleftherios Gkioulekas , 2008
"... In this paper, we revisit the claim that the Eulerian and quasi-Lagrangian same time correlation tensors are equal. This statement allows us to transform the results of an MSR quasi-Lagrangian statistical theory of hydrodynamic turbulence back to the Eulerian representation. We define a hierarchy of ..."
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In this paper, we revisit the claim that the Eulerian and quasi-Lagrangian same time correlation tensors are equal. This statement allows us to transform the results of an MSR quasi-Lagrangian statistical theory of hydrodynamic turbulence back to the Eulerian representation. We define a hierarchy of homogeneity symmetries between the local homogeneity of Frisch and global homogeneity. It is shown that both the elimination of the sweeping interactions and the derivation of the 4/5-law require a homogeneity assumption stronger than local homogeneity but weaker than global homogeneity. The quasi-Lagrangian transformation, on the other hand, requires an even stronger homogeneity assumption which is many-time rather than one-time but still weaker than many-time global homogeneity. We argue that it is possible to relax this stronger assumption and still preserve the conclusions derived from theoretical work based on the quasi-Lagrangian transformation.

On the elimination of the sweeping interactions from theories of hydrodynamic turbulence

by Eleftherios Gkioulekas , 2006
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The effect of asymmetric large-scale dissipation on energy and potential enstrophy injection in two-layer quasi-geostrophic turbulence

by Eleftherios Gkioulekas - UNDER CONSIDERATION FOR PUBLICATION IN J. FLUID MECH. , 2011
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Under consideration for publication in J. Fluid Mech. 1 An Inequality between Fluxes of Energy and Enstrophy in 2D and QG Turbulence

by Kit Tung, Eleftherios Gkioulekas , 2004
"... In systems governing two-dimensional turbulence, surface quasi-geostrophic turbulence, (more generally α-turbulence), two-layer quasi-geostrophic turbulence, etc., there often exist two conservative quadratic quantities, one “energy”-like and one “enstrophy”-like. In a finite inertial range there ar ..."
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In systems governing two-dimensional turbulence, surface quasi-geostrophic turbulence, (more generally α-turbulence), two-layer quasi-geostrophic turbulence, etc., there often exist two conservative quadratic quantities, one “energy”-like and one “enstrophy”-like. In a finite inertial range there are in general two spectral fluxes, one associated with each conserved quantity. The energy spectrum in general has a contribution from each of the fluxes, and our previous work showed that these two contributions to the energy spectrum can be linearly superimposed despite the highly nonlinear nature of the problem. Often, one of the fluxes is dominant and the energy spectrum then has the visual shape of the case with a single flux; the contribution from the subdominant flux is effectively hidden. The relative magnitudes of the spectral fluxes depend on the dissipative sinks in the system, and varies according to the physical/mathematical system under consideration. We derive an important inequality involving the “energy ” and enstrophy ” fluxes for each representative system. This result then allows us to determine the effective energy spectral shape in the general case of double cascades. 1.

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by unknown authors , 2006
"... A new proof on net upscale energy cascade in two-dimensional and quasi-geostrophic turbulence ..."
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A new proof on net upscale energy cascade in two-dimensional and quasi-geostrophic turbulence

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by Eleftherios Gkioulekas A , 2006
"... On the elimination of the sweeping interactions from theories of hydrodynamic turbulence ..."
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On the elimination of the sweeping interactions from theories of hydrodynamic turbulence
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... in the limit of infinite Reynolds number. For the case of finite Reynolds number, there is a homogeneous and particular solution to the generalized structure functions that are linearly superimposed =-=[81, 82]-=-. Then the calculation of ζ3 is relevant only for the homogeneous solution. Aside from this issue, this argument too requires that we set I2 = 0. Dropping I2 cannot be justified under local homogeneit...

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