UFR 3-06 References: Difference between revisions
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{{UFR|front=UFR 3-06|description=UFR 3-06 Description|references=UFR 3-06 References|testcase=UFR 3-06 Test Case|evaluation=UFR 3-06 Evaluation|qualityreview=UFR 3-06 Quality Review|bestpractice=UFR 3-06 Best Practice Advice|relatedACs=UFR 3-06 Related ACs}} | {{UFR|front=UFR 3-06|description=UFR 3-06 Description|references=UFR 3-06 References|testcase=UFR 3-06 Test Case|evaluation=UFR 3-06 Evaluation|qualityreview=UFR 3-06 Quality Review|bestpractice=UFR 3-06 Best Practice Advice|relatedACs=UFR 3-06 Related ACs}} | ||
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= Natural and mixed convection boundary layers on | = Natural and mixed convection boundary layers on vertical heated walls (A) = | ||
Underlying Flow Regime 3-06 <font size="-2" color="#888888"> © copyright ERCOFTAC 2004</font> | Underlying Flow Regime 3-06 <font size="-2" color="#888888"> © copyright ERCOFTAC 2004</font> | ||
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16. S.Thangam, R.Abid, G.G.Speziale (1992), Application of a new (k, ô) model to near wall turbulent flows, AIAA J. 30, 552-554. | 16. S.Thangam, R.Abid, G.G.Speziale (1992), Application of a new (k, ô) model to near wall turbulent flows, AIAA J. 30, 552-554. | ||
<font size="-2" color="#888888">© copyright ERCOFTAC 2004</font><br /> | <font size="-2" color="#888888">© copyright ERCOFTAC 2004</font><br /> | ||
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Contributors: André Latrobe - CEA / DRN / Department de Thermohydraulique | Contributors: André Latrobe - CEA / DRN / Department de Thermohydraulique | ||
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{{UFR|front=UFR 3-06|description=UFR 3-06 Description|references=UFR 3-06 References|testcase=UFR 3-06 Test Case|evaluation=UFR 3-06 Evaluation|qualityreview=UFR 3-06 Quality Review|bestpractice=UFR 3-06 Best Practice Advice|relatedACs=UFR 3-06 Related ACs}} | {{UFR|front=UFR 3-06|description=UFR 3-06 Description|references=UFR 3-06 References|testcase=UFR 3-06 Test Case|evaluation=UFR 3-06 Evaluation|qualityreview=UFR 3-06 Quality Review|bestpractice=UFR 3-06 Best Practice Advice|relatedACs=UFR 3-06 Related ACs}} | ||
Latest revision as of 12:52, 12 February 2017
Natural and mixed convection boundary layers on vertical heated walls (A)
Underlying Flow Regime 3-06 © copyright ERCOFTAC 2004
References
1. D.P.Mikielewicz, A.M.Shehata, J.D.Jackson, D.M.McEligot (2002) Temperature, velocity and mean turbulence structure in strongly heated internal gas flows. Comparisons of numerical predictions with data, International Journal of Heat and mass transfer 45, 4333- 4352
2. S.I.Satake, T.Kunugi, A.M.Shehata, D.M.McEligot (2000) Direct numerical simulation for laminarization of turbulent forced gas flows in circular tubes with strong heating, International Journal of Heat and Fluid Flow 21, 526-534
3. A.M.Shehata, D.M.McEligot (1998) Mean structure in the viscous sublayer of strongly heated internal gas flows. Measurements, International Journal of Heat and mass transfer 41, 4297-4313
4. L.V Humble, W.H Lowdermilk, L.G Desmon (1951) Measurement of averaged heat transfer and friction coefficients for subsonic flow of air in smooth tubes at high surface and fluid temperatures, NACA report 1020.
5. J.D. Jackson (1961): A theoretical investigation into the effects of surface/gas temperature ratio for fully developed turbulent flow of air, helium and carbon dioxide in smooth circular tubes ARC 22, 784, F.M.3084 (UK).
6. D.M McEligot, P.M Magee, G.Leppert (1965), Effect of large temperature gradients on convective heat transfer : the downstream region, J. Heat Transfer 87, 67-76.
7. H.C Perkins, P.M Worsoe-Schmidt (1965) Turbulent heat and momentum transfer for gases in a circular tube at wall to bulk temperature ratios to seven, , International Journal of Heat and mass transfer 8, 1011-1031
8. C.A.Bankston,D.M.McEligot (1970), Turbulent and laminar heat transfer to gases with varying properties in the entry region of circular ducts, , International Journal of Heat and mass transfer 13, 319-344
9. M.A.Cotton (1987), Theoretical studies of mixed convection in vertical tubes, PhD thesis, University of Manchester.
10 W.P.Jones, B.E.Launder (1973), The calculation of low Reynolds number phenomena with a two equation model of turbulence, International Journal of Heat and mass transfer 16, 1119-1130
11..B.E.Launder, B.I.Sharma (1974) Application of the energy dissipation model of turbulence to the calculation of flow near a spinning disc, Lett. Heat Transfer 1, 131-138
12. K.Y.Chen, (1982) Predictions of channel and boundary layer flows with a low Reynolds number turbulence model, AIAA J. 20, 33-38
13. C.K.G. Lam, K.A. Bremhorst, (1981) Modified form of the (k, å) model for predicting wall turbulence, J.Fluids Engineering 103, 456-460
14. V.Michelassi, W.Rodi, G.Scheuerer, (1991) Testing a low Reynolds number (k, å) turbulence model based on direct simulation data. U.Karlsruhe, manuscript presented at Eighth symposium on turbulent shear flows, München.
15. T.H.Shi, A.T. Hsu (1991), An improved (k, å) model for near wall turbulence, AIAA paper 91-0611.
16. S.Thangam, R.Abid, G.G.Speziale (1992), Application of a new (k, ô) model to near wall turbulent flows, AIAA J. 30, 552-554.
© copyright ERCOFTAC 2004
Contributors: André Latrobe - CEA / DRN / Department de Thermohydraulique