Using measurements of all three components of the temperature dissipation χ in a laboratory boundary layer, the measured probability density p (χr) of χr, or χ averaged over a distance r, is found to be closely log-normal over a significant range of r. The variance σ2 of lnχr follows the relation σ2=A+μln(L/r), with μ=0.35, where L is an integral scale of turbulence. High order moments, up to order 5, of χr show a power-law variation with r/L. With increasing order of the moment, the power-law exponents become increasingly smaller than the corresponding values implied by assumed log-normality of p (χr) but are consistent with the bounds given by Novikov’s theory. It is suggested that the observed close agreement with log-normality of p (χr) may be misleading when sufficiently high order moments of χr are considered.
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Antonia et al. (1977) studied this question.
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