𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Karhunen–Loeve representations of turbulent channel flows using the method of snapshots

✍ Scribed by R. A. Handler; K. D. Housiadas; A. N. Beris


Publisher
John Wiley and Sons
Year
2006
Tongue
English
Weight
446 KB
Volume
52
Category
Article
ISSN
0271-2091

No coin nor oath required. For personal study only.


📜 SIMILAR VOLUMES


Applications of the artificial compressi
✍ J. W. Lee; M. D. Teubner; J. B. Nixon; P. M. Gill 📂 Article 📅 2005 🏛 John Wiley and Sons 🌐 English ⚖ 406 KB

## Abstract A three‐dimensional (3‐D) numerical method for solving the Navier–Stokes equations with a standard __k–ε__ turbulence model is presented. In order to couple pressure with velocity directly, the pressure is divided into hydrostatic and hydrodynamic parts and the artificial compressibilit

Simulation of unsteady turbulent flows a
✍ K. J. Badcock; F. Cantariti; I. Hawkins; M. Woodgate; L. Dubuc; B. E. Richards 📂 Article 📅 2000 🏛 John Wiley and Sons 🌐 English ⚖ 275 KB 👁 2 views

The pseudo-time formulation of Jameson has facilitated the use of numerical methods for unsteady flows, these methods have proved successful for steady flows. The formulation uses iterations through pseudo-time to arrive at the next real time approximation. This iteration can be used in a straightfo

Prediction of turbulent gas–solids flow
✍ S. Naik; I.G. Bryden 📂 Article 📅 1999 🏛 John Wiley and Sons 🌐 English ⚖ 230 KB 👁 2 views

The flow of particulate two-phase flow mixtures occur in several components of solid fuel combustion systems, such as the pressurised fluidised bed combustors (PFBC) and suspension-fired coal boilers. A detailed understanding of the mixture characteristics in the conveying component can aid in refin

Simulations of the turbulent channel flo
✍ Volker John; Michael Roland 📂 Article 📅 2007 🏛 John Wiley and Sons 🌐 English ⚖ 437 KB

## Abstract Projection‐based variational multiscale (VMS) methods, within the framework of an inf–sup stable second order finite element method for the Navier–Stokes equations, are studied in simulations of the turbulent channel flow problem at __Re__~τ~ = 180. For comparison, the Smagorinsky large