We perform large-eddy simulations of incompressible, fully developed turbulent flow in a square duct bounded above by a free-slip wall, for Reynolds numbers based on the mean friction velocity and the duct width equal to 360, 600 and 1000. The flow in the corner is strongly affected by the advection due to two counter-rotating secondary flow regions present immediately below the free surface, an inner one close to the corner, and an outer one. Because of the convection of the inner eddy, as the free surface is approached the friction velocity on the side wall first decreases, then increases again. A similar behavior is observed for the surface-parallel Reynolds-stress components. The budgets of the Reynolds stresses show a strong reduction of all terms of the dissipation tensor in both the inner and outer near-corner region. The turbulent-kinetic energy budget exhibits a reduction in both production and dissipation towards the free surface. The turbulent kinetic energy production and the surface-parallel fluctuations rebound in the thin layer adjacent to the free surface. The Reynolds-stress anisotropy appears to be the main factor in the generation of the mean secondary flow. The multi-layer structure of the boundary-layer near the free surface is also discussed.
Large-eddy simulation of wall-bounded flows with a free surface
R Broglia;
2002
Abstract
We perform large-eddy simulations of incompressible, fully developed turbulent flow in a square duct bounded above by a free-slip wall, for Reynolds numbers based on the mean friction velocity and the duct width equal to 360, 600 and 1000. The flow in the corner is strongly affected by the advection due to two counter-rotating secondary flow regions present immediately below the free surface, an inner one close to the corner, and an outer one. Because of the convection of the inner eddy, as the free surface is approached the friction velocity on the side wall first decreases, then increases again. A similar behavior is observed for the surface-parallel Reynolds-stress components. The budgets of the Reynolds stresses show a strong reduction of all terms of the dissipation tensor in both the inner and outer near-corner region. The turbulent-kinetic energy budget exhibits a reduction in both production and dissipation towards the free surface. The turbulent kinetic energy production and the surface-parallel fluctuations rebound in the thin layer adjacent to the free surface. The Reynolds-stress anisotropy appears to be the main factor in the generation of the mean secondary flow. The multi-layer structure of the boundary-layer near the free surface is also discussed.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
