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

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