Program NATCON: for the numerical solution of buoyancy-driven laminar and turbulent flows in differentially heated cavities

469 635 415 3 4447 document 415 Program_Natcon_Reportr2.pdf application/pdf 581071 2011-09-09 10:20:17 https://vuir.vu.edu.au/469/1/Program_Natcon_Reportr2.pdf 469 1 application/pdf text en public

Program_Natcon_Reportr2.pdf

http://eprints.org/relation/hasVolatileVersion https://vuir.vu.edu.au/id/document/10683 http://eprints.org/relation/hasVersion https://vuir.vu.edu.au/id/document/10683 http://eprints.org/relation/hasIndexCodesVersion https://vuir.vu.edu.au/id/document/10683 10683 3 1734424 document 10683 indexcodes.txt text/plain 0af718ec28e07aeb77ff71b78fee7c43 MD5 11757 2013-02-06 17:10:11 https://vuir.vu.edu.au/469/2/indexcodes.txt 469 2 2 text/plain other Generate index codes conversion from application/pdf to indexcodes en public

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http://eprints.org/relation/isVersionOf https://vuir.vu.edu.au/id/document/415 http://eprints.org/relation/isVolatileVersionOf https://vuir.vu.edu.au/id/document/415 http://eprints.org/relation/issmallThumbnailVersionOf https://vuir.vu.edu.au/id/document/415 archive 39 disk0/00/00/04/69 2006-08-17 2021-08-27 07:39:44 2008-08-19 21:02:11 other show Prakash Mahesh Turan Ozden Thorpe Graham R Program NATCON: for the numerical solution of buoyancy-driven laminar and turbulent flows in differentially heated cavities unpub 230000 290000 tafeengineering convection, natural, turbulent, cavity, cfd The report correlates the partial differential equations that govern buoyancy-driven laminar and turbulent flows in differentially heated cavities. It is shown how the equations are discretised on a non-uniform mesh and then solved. The k-epsilon model has been used to represent the effects of turbulence and its low Reynolds number formulation has been used so the equations may be integrated close to the wall. It is intended that the work will provide a bridge between theory and practice, and be useful to researchers relative new to the area of computational fluid dynamics. 2006-08 published Victoria University public UNSPECIFIED Ampofo, F. and Karayiannis, T. G. (2003) Experimental benchmark data for turbulent natural convection in an air filled square cavity. Int. J. Heat and Mass Transfer, 46, 3551-3572. Chien, K. Y., (1982) Predictions of channel and boundary layer flows with a low Reynolds number turbulence model. AIAA Journal, 20, 33-38. Craft T. J., Gerasimov A. V., Iacovides H. and Launder B. E. (2002) Progress in the Generalization of Wall-Function Treatments, Int. J. Heat and Fluid Flow, 23, No. 2, pp. 148-160. Gray, D. D. and Giorgini, A. (1976) The validity of the Boussinesq approximation for liquids and gases. International Journal of Heat and Mass Transfer, 24, 125-131. Harlow, F. H. and Nakayama, P. (1967) Turbulence transport equations. Physics of Fluids, 11, 2323-2332. Harlow, F. H. and Welch, J. E. (1965) Numerical calculation for time dependent viscous incompressible flow of fluid with free surface. Physics of Fluids, 8, 2182-2189. Henkes, R. A. W. M. (1990) Natural-Convection Boundary Layers. Ph.D. thesis, Technical University of Delft, The Netherlands. Jones, W. P. and Launder, B. E. (1972) The Prediction of laminarization with a two-equation model of turbulence. International Journal of Heat and Mass Transfer, 15, 301-314. Patankar, S. V. and Spalding, D. B., (1972) A Calculation Procedure for Heat, Mass and Momentum Transfer in Three Dimensional Parabolic Flows, International Journal of Heat and Mass Transfer, 15, p.1787. Patankar, S. V. (1980) Numerical Heat Transfer and Fluid Flow. Hemisphere Publishing Corporation, Washington. Wilcox, D. C. (1993) Turbulence Modelling for CFD. DCW Industries, La Canada. FALSE