In terms of a dimensionless number, ΠNRa/1+Pr1, introduced by Arpacı (1986, 1990, 1995) for buoyancy driven flows, Ra and Pr respectively being the usual Rayleigh and Prandtl numbers, two well-known correlations (Churchill and Chu, 1975) for natural convection next to a vertical isothermal plate are reduced in terms of ΠL=Ra/1+0.492Pr1 to Nu=0.67ΠL1/4,103ΠL109, for the laminar case, and in terms of ΠT=Ra/1+0.164Pr1 to Nu=0.15ΠT1/3,109ΠT1012, for the turbulent case.

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