Abstract

Abstract A two-dimensional numerical model is used to calculate the nonlinear evolution of Kelvin-Helmholtz (KH) billows for various Reynolds numbers in the range where the turbulent collapse of the waves is expected. The onset of disordered motions is not observed in these numerical experiments, presumably because the transition requires the third spatial degree of freedom. Although we have shown elsewhere that these two-dimensional KH wave states are unstable with respect to three-dimensional perturbations, the spanwise coherent large-scale structure is observed to persist in presence of the small-scale fluctuations. Thus the two-dimensional wave structure is of importance in itself and the present paper is devoted to a detailed study of the laminar evolution of the dominant large-scale vortices. An analysis of the transfer of energy between the wave and the mean flow firmly establishes that the wave does not enter a steady state upon achieving maximum amplitude. Rather, it begins an almost periodic exc...

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