Abstract.
Intermittency, measured as \(\log \left({F(r)}/{3}\right)\), where F(r) is the flatness of velocity increments at scale r, is found to rapidly increase as viscous effects intensify, and eventually saturate at very small scales. This feature defines a finite intermediate range of scales between the inertial and dissipation ranges, that we shall call near-dissipation range. It is argued that intermittency is multiplied by a universal factor, independent of the Reynolds number Re, throughout the near-dissipation range. The (logarithmic) extension of the near-dissipation range varies as \(\sqrt{\log Re}\). As a consequence, scaling properties of velocity increments in the near-dissipation range strongly depend on the Reynolds number.
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Chevillard, L., Castaing, B. & Lévêque, E. On the rapid increase of intermittency in the near-dissipation range of fully developed turbulence. Eur. Phys. J. B 45, 561–567 (2005). https://doi.org/10.1140/epjb/e2005-00214-4
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DOI: https://doi.org/10.1140/epjb/e2005-00214-4