Abstract
The dynamic subgrid‐scale eddy viscosity model has been used in the large‐eddy simulation of the turbulent flow in a plane channel for Reynolds numbers based on friction velocity and channel half‐width ranging between 200 and 2000, a range including values significantly higher than in previous simulations. The computed wall stress, mean velocity, and Reynolds stress profiles compare very well with experimental and direct simulation data. Comparison of higher moments is also satisfactory. Although the grid in the near‐wall region is fairly coarse, the results are quite accurate: the turbulent kinetic energy peaks at y+≂12, and the near‐wall behavior of the resolved stresses is captured accurately. The model coefficient is o(10−3) in the buffer layer and beyond, where the cutoff wave numbers are in the decaying region of the spectra; in the near‐wall region the cutoff wave numbers are nearer the energy‐containing range, and the resolved turbulent stresses become a constant fraction of the resolved stresses. This feature is responsible for the correct near‐wall behavior of the model coefficient. In the near‐wall region the eddy viscosity is reduced to account for the energy transfer from small to large scales that may occur locally.