A nonlocal expression for the turbulent Reynolds stress u ′ v ′ ¯ solves in a unified manner for the velocity profiles in jets, shear layers, wakes, and boundary layers, offering predictions consistent with known measurements in these canonical flows. The framework is the random walk inspired closure of Prandtl (1925) since we write u ′ v ′ ¯=-v ˜ℓ∂ y u with ℓ a mean free path but, by contrast with Prandtl, with v ˜ a nonlocal transfer velocity resulting from an integration over an appropriate portion of space of the mean velocity profile u(y). The status of ℓ is discussed and its value, a fraction (10π) -1 ≈0.031 of the integral scale, is computed in opened shear flows. The closure is adapted to the special case of boundary layers, where the value of the von Kármán constant is found to be κ=6 -1/2 ≈0.41.
Emmanuel Villermaux (Fri,) studied this question.
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