Abstract
In light of some recent experiments on quasi two-dimensional (2D) turbulent channel flow we provide here a model of the ideal case, for the sake of comparison. The ideal 2D channel flow differs from its three-dimensional (3D) counterpart by having a second quadratic conserved variable in addition to the energy and the latter has an inverse rather than a direct cascade. The resulting qualitative differences in profiles of velocity V and energy K as a function of the distance from the wall are highlighted and explained. The most glaring difference is that the 2D channel is much more energetic, with K in wall units increasing logarithmically with the Reynolds number Ret instead of being Ret independent in 3D channels.
Original language | English |
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Article number | 045304 |
Pages (from-to) | 045304-1/4 |
Number of pages | 4 |
Journal | Physical Review E - Statistical, Nonlinear, and Soft Matter Physics |
Volume | 79 |
Issue number | 4 |
DOIs | |
Publication status | Published - 2009 |