The relation, first written by Kolmogorov, between the third-order moment of the longitudinal velocity increment δu 1 and the second-order moment of δu 1 is presented in a slightly more general form relating the mean value of the product δu 1 ( δu i ) 2 , where ( δu i ) 2 is the sum of the square of the three velocity increments, to the secondorder moment of δu i . In this form, the relation is similar to that derived by Yaglom for the mean value of the product δu 1 ( δu θ ) 2 where ( δu θ ) 2 is the square of the temperature increment. Both equations reduce to a ‘four-thirds’ relation for inertialrange separations and differ only through the appearance of the molecular Prandtl number for very small separations. These results are confirmed by experiments in a turbulent wake, albeit at relatively small values of the turbulence Reynolds number.
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Antonia et al. (1997) studied this question.
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