Abstract

AbstractIn this study, a benchmark natural convection problem is studied under a Gay–Lussac‐type approximation incorporating centrifugal effects in the context of a new vorticity‐stream‐function approach. This approximation differs from the classic Boussinesq approximation in that density variations are considered in the advection term as well as the gravity term in the momentum equations. Such a treatment invokes Froude number as a non‐Boussinesq parameter deviating results from the classic Boussinesq approximation. It is also shown how the Gay–Lussac parameter may be expressed by its equivalent relative temperature difference. Numerical simulation of natural convection in square and skewed cavities are performed up to Ra = 106 and ϵ = 0.3 at Pr = 0.71. Results obtained with new approximation are compared against the weakly compressible approach and the conventional Boussinesq approximation in terms of the average and local Nusselt number, coefficient of friction and entropy generation. Comparing the local Nusselt number indicates a negligible difference between Gay–Lussac type and the Boussinesq approximations even at a high relative temperature difference, with both deviating from the weakly compressible approach. Comparing coefficient friction results obtained by the Gay–Lussac‐type approximation against the weakly compressible approach confirms superior numerical data in some regions of the physical domain with less deviation for rotating flows in comparison with the Boussinesq approximation. Finally, comparing the computational cost of the numerical simulation shows at least 8% less computational cost when governing equations are solved via secondary variables using a central scheme rather than primitive variables.

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