Langevin and diffusion equation of turbulent fluid flow
Author(s) -
J.J.H. Brouwers
Publication year - 2010
Publication title -
physics of fluids
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.188
H-Index - 180
eISSN - 1089-7666
pISSN - 1070-6631
DOI - 10.1063/1.3466658
Subject(s) - physics , langevin equation , turbulence , reynolds number , turbulent diffusion , eulerian path , classical mechanics , kolmogorov microscales , mean squared displacement , statistical physics , mechanics , k epsilon turbulence model , k omega turbulence model , mathematical physics , lagrangian , quantum mechanics , molecular dynamics
A derivation of the Langevin and diffusion equations describing the statistics of fluid particle displacement and passive admixture in turbulent flow is presented. Use is made of perturbation expansions. The small parameter is the inverse of the Kolmogorov constant C0, which arises from Lagrangian similarity theory. The value of C0 in high Reynolds number turbulence is 5–6. To achieve sufficient accuracy, formulations are not limited to terms of leading order in C0−1 including terms next to leading order in C0−1 as well. Results of turbulence theory and statistical mechanics are invoked to arrive at the descriptions of the Langevin and diffusion equations, which are unique up to truncated terms of O(C0−2) in displacement statistics. Errors due to truncation are indicated to amount to a few percent. The coefficients of the presented Langevin and diffusion equations are specified by fixed-point averages of the Eulerian velocity field. The equations apply to general turbulent flow in which fixed-point Euleri...
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