Abstract
The temporal formation of the buoyancy-driven flow structures in a bottom heated, shallow, cylindrical fluid layer was numerically studied. The unsteady three-dimensional Navier-Stokes and energy equations were discretized by the power law scheme and solved by the fully implicit Marker-and-Cell method. Computations were carried out for the pressurized argon (Pr = 0.69) and water (Pr = 6.1) layers for various Rayleigh numbers and heating rates of the layer. In the pressurized argon layer at a slightly supercritical Rayleigh number with Ra{sub f} = 1.05Ra{sub c} a steady straight roll pattern was formed when the heating rate was very slow (a = 0.001) after a long transient stage. When the heating rate was raised to a = 0.01, a very different structure like U-rolls was formed at steady state. In the water layer with Ra{sub f} = 1.05Ra{sub c}, a straight roll pattern was again formed, but at a = 0.01. At Ra{sub f} = 1.13Ra{sub c}, curved rolls with the three foci at the sidewall were formed for a = 0.01. A pattern in the form of U-rolls appears at a = 0.01. Regular concentric circular rolls prevail at a = 1.0. When the Rayleigh number is further raised tomore » 1.23Ra{sub c}, the resulting steady flow is dominated by incomplete circular rolls with open ends near {theta} = 0{degree}.« less
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