Kármán–Howarth equation
Mathematical equation / From Wikipedia, the free encyclopedia
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In isotropic turbulence the Kármán–Howarth equation (after Theodore von Kármán and Leslie Howarth 1938), which is derived from the Navier–Stokes equations, is used to describe the evolution of non-dimensional longitudinal autocorrelation.[1][2][3][4][5]