UFR 3-12 References: Difference between revisions
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[1] The prediction of the mean flow in the vicinity of the stagnation point of e.g. a bluff body is not affected. | |||
Revision as of 16:53, 11 March 2009
Stagnation point flow
Underlying Flow Regime 3-12 © copyright ERCOFTAC 2004
References
Camci, C., Arts, T. (1985a), "Short Duration Measurements and Numerical Simulation of Heat Transfer Along the Suction Side of a Film-Cooled Gas Turbine Blade", J. Eng. Power, 107, 991 997.
Camci, C., Arts, T. (1985b), "Experimental Heat Transfer Investigation Around the Film-Cooled Leading Edge of a High-Pressure Gas Turbine Blade", J. Eng. Power, 107, 1016 1021.
Camci, C., Arts, T. (1990), "An Experimental Convective Heat Transfer Investigation Around a Film-Cooled Gas Turbine Blade", J. Eng. Power, 112, 497 503.
Consigny, H,. Richards, B.E. (1983), "Short Duration Measurements of Heat Transfer Rate to a Gas Turbine Rotor Blade", ASME Journal of Engineering for Power, Vol. 104, No. 3, July, pp. 542 - 551
Durbin, P. A. (1996), "On the k-3 Stagnation Point Anomaly", Int. J. Heat and Fluid Flow, 17, 1, 89 90.
Laurence, D. (2002), "Applications of Reynolds Averaged Navier Stokes Equations to Industrial Flows", Von Karman Inst. Lect. Series: Introduction to Turbulence Modelling.
Kato, M., Launder, B.E. (1993), "The Modelling of Turbulent Flow Around Stationary and Vibrating Square Cylinders", 9th Symposium on Turbulent Shear Flows, Kyoto, Japan, August 16-18, pp. 10-4-1 10-4-6
Køllgaard Voigt, L. (2000), "Comparison of Turbulence Models for Numerical Calculation of Airflow in an Annex 20 Room", International Center for Indoor Environment and Energy, Dept. of Energy Engineering, Tech. University of Denmark, http://www.ie.dtu.dk/prev_res_results/January00.asp
Kral, L.D., Mani, M. and Ladd, J. (1996), "Application of Turbulence Models for Aerodynamic and Propulsion Flowfields", AIAA J., 34, 11, 2291 2298.
Ligrani, P.M., Camci, C., Grady, M.S. (1982) "Thin Film Heat Transfer Gauge Construction and Measurement Details", VKI TM 33, November
Medic, G. (2001), "Flow Problem Without Cooling", http://www.stanford.edu/~gmedic/cooling1.html
Medic, G., Durbin, P.A. (2002), "Toward Improved Prediction of Heat Transfer on Turbine Blades", J. Turbomach.-Trans. ASME, 124, 2, 187 192. http://www.stanford.edu/ ~gmedic/
Menter, F.R. (1992), "Influence of Freestream Values on k-ω Turbulence Model Predictions", AIAA J., 30, 6, 1657 1659.
Menter, F.R. (1994), "Two-Equation Eddy-Viscosity Turbulence Models for Engineering Applications", AIAA J., 32, 8, 1598 1605.
Menter, F.R., Grotjans, H., Unger, F. (1997), "Numerical Aspects of Turbulence Modelling for Reynolds Averaged Navier-Stokes Equations", Von Karman Inst. Lect. Series 1997-02 on Computational Fluid Dynamics, Rhode Saint Genese.
Rodi, W. and Scheurer, G. (1986), "Scrutinizing the k-ε Turbulence Model under Adverse Pressure Gradient Conditions", ASME J. Fluid Eng., 108, 174 179.
Schultz, D.L., Jones, T.V. (1973) "Heat Transfer Measurements in Short Duration on Hypersonic Facilities", AGARDograpg 165
STAR-CD, Version 3.10 Methodology, 1999, Computational Dynamics Limited.
Strahle, W.C. (1985), "Stagnation Point Flows with Freestream Turbulence The Matching Condition", AIAA J., 23, 11, 1822 1824.
Versteeg, H.K., Malalasekera, W. (1996), "Turbulence and its Modelling", An Introduction to Computational Fluid Dynamics, Chapter 3, Longman.
Yakhot, V., Orszag, S.A., Tangham, S., Gatski, T.B. and Speciale, C.G. (1992), "Development of Turbulence Models for Shear Flows by a Double Expansion Technique", Phys. Fluids, A4 (7).
Wilcox, D.C., (1993), Turbulence modeling for CFD, La Cañada, California.
[1] The prediction of the mean flow in the vicinity of the stagnation point of e.g. a bluff body is not affected.
© copyright ERCOFTAC 2004
Contributors: Beat Ribi - MAN Turbomaschinen AG Schweiz