An exact expression for the Reynolds number dependence of the energy dissipation rate in homogeneous, isotropic turbulence

Physics – Fluid Dynamics

Scientific paper

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10 pages, 1 figure

Scientific paper

The Reynolds number dependence of the dimensionless dissipation rate is derived directly from the Karman-Howarth equation in terms of the inverse of the integral scale Reynolds number and a coefficient which depends on the second- and third-order structure functions. Fitting this form to the results from a direct numerical simulation indicates that the coefficient is effectively constant.

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