2009
DOI: 10.1007/s12043-009-0096-6
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Statistical properties of turbulence: An overview

Abstract: Abstract. We present an introductory overview of several challenging problems in the statistical characterisation of turbulence. We provide examples from fluid turbulence in three and two dimensions, from the turbulent advection of passive scalars, turbulence in the one-dimensional Burgers equation, and fluid turbulence in the presence of polymer additives.

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Cited by 65 publications
(82 citation statements)
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References 142 publications
(199 reference statements)
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“…We are interested in 2D incompressible fluids, so we use the following stream-function-vorticity formulation363738 for the momentum equation:…”
Section: Resultsmentioning
confidence: 99%
“…We are interested in 2D incompressible fluids, so we use the following stream-function-vorticity formulation363738 for the momentum equation:…”
Section: Resultsmentioning
confidence: 99%
“…In turbulent flows, the non-Newtonian nature of polymer solutions manifests itself through a considerable reduction of the turbulent drag compared to that of the solvent alone [2][3][4][5][6]. What renders this phenomenon even more remarkable is that an appreciable drag reduction can already be observed at very small polymer concentrations (of the order of a few parts per million).…”
Section: Introductionmentioning
confidence: 99%
“…For equal-time structure functions, multiscaling means that the scaling exponents are a nonlinear, convex, monotonically increasing function of p and not a linear function as suggested by simple dimensional analysis [6,17]. Given the large range of scales that we can cover in this shell model [18], E b ðkÞ reveals two distinct, power-law ranges.…”
mentioning
confidence: 99%
“…We show that a shell-model version of the 3D Hall-MHD equations [11,12], which is a generalization of MHD shell models [14][15][16], provides a natural theoretical model for investigating such multiscaling behaviors in structure functions. For equal-time structure functions, multiscaling means that the scaling exponents are a nonlinear, convex, monotonically increasing function of p and not a linear function as suggested by simple dimensional analysis [6,17]. Given the large range of scales that we can cover in this shell model [18], E b ðkÞ reveals two distinct, power-law ranges.…”
mentioning
confidence: 99%