Titlebook: Direct and Large-Eddy Simulation IV; Bernard J. Geurts,Rainer Friedrich,Olivier Métais Book 2001 Springer Science+Business Media Dordrecht

miniature

Wolfgang Buck,Steffen Rudtsch Dr.an direction than the mesh employed for a discretization of the resolved quantities. The truncated NavierStokes equations are solved through a sequence of runs, each initialized using the subgrid-scale estimation model. The modeling procedure is illustrated on the example of forced and decaying isotropic turbulence.

Fretful

串通

incredulity

Large Eddy Simulations Using the Subgrid-Scale Estimation Model and Truncated Navier-Stokes Dynamican direction than the mesh employed for a discretization of the resolved quantities. The truncated NavierStokes equations are solved through a sequence of runs, each initialized using the subgrid-scale estimation model. The modeling procedure is illustrated on the example of forced and decaying isotropic turbulence.

Lacerate

潜移默化

Large Eddy Simulation of Flow Around a High Lift Airfoil,achment and a separation near the trailing edge. To handle this high Reynolds number flow with LES on available supercomputers, a local mesh refinement technology and a low dissipative scheme are developed. It appears that the computed mean and fluctuating velocity profiles compare reasonably well with experimental measurements.

adumbrate

vitreous-humor

floaters

Precision Machinery Using MEMS Technologyulent flame speed with increasing turbulent intensity at the position of the flame front, which is in good agreement with experimental and theoretical data. The turbulent flame speed also shows a dependence of the expansion coefficient and increases with higher expansion rates.

Obstruction