Titlebook: Recent Advances in DNS and LES; Proceedings of the S Doyle Knight,Leonidas Sakell Conference proceedings 1999 Springer Science+Business Med

Glower

Fluid Mechanics and Its Applicationshttp://image.papertrans.cn/r/image/822700.jpg

Canopy

https://doi.org/10.1007/978-94-011-4513-83D; algorithm; algorithms; layers; linear optimization; model; modeling; modelling; simulation

overreach

Large-Eddy Simulations of Compressible Shear Flows). Quasi-incompressible transitional boundary layers show the establishement of a streak system of spanwise spacing ~ 100. well upstream of the peak of skin friction, which bolsters up the expanations in terms of algebraic instabilities (e.g. Landahl, 1980, ., ., 243–251). A supersonic compression-r

habile

Perigee

Direct Navier-Stokes Simulation of Sounds Generatei by Shock-Vortex / Vortex-Vortex Interactions and propagation mechanisms of sounds are studied. The unsteady, compressible Navier-Stokes equations are solved by a finite difference method over the entire acoustic field from near to far fields. The sixth-order-accurate compact Padé scheme is used for spatial derivatives, together with the fourt

矛盾心理

殘忍

沒有貧窮

Modelling of the Length Scale and Variance of Subgrid Scale Quantities in a Turbulent Channel Flowth with and without system rotation. From these simulations subgrid scale (SGS) quantities are evaluated and compared with SGS model predictions in . tests. Although the mean behaviour of the SGS dissipation is captured relatively well by the Smagorinsky model, the variation of the modelled SGS diss

壕溝

DNS of Compressible Reacting Mixing Layers with Parallel Compact Schemerecent understanding of the three-mode mixing mechanism. The extension of the foregoing is of interest but requires the implementation of high-order finite difference formulas on supercomputers in order to take advantage of the massive parallelization. The high-order differencing and filtering formu

施舍

Large Eddy Simulation of Stationary Premixed Flames Using a Subgrid Flamelet Approacheering combustor. Flamelet type combustion is assumed for both types of flames and experimental conditions are used for the simulations. The geometric characteristics of the flame surfaces and their effects on fluid dynamics are well predicted for the former type of flames. For the combustor simulat