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Chapter 10: Natural Convection Gas Transport in Porous Media
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                           Nusselt and Sherwood numbers are deduced. For some particular cases, quantita-
                           tive comparisons with previous works reported in the literature were reported and
                           the agreement between theoretical results and experimental data was found to be
                           satisfactory.
                             A mathematical model governing free convection boundary-layer flow over an
                           isothermal inclined plate embedded in a thermally stratified porous medium in the
                           presence of a non-uniform transverse magnetic field was developed by Chamkha
                           (1997b). The resulting equations of that study account for non-Darcian boundary and
                           inertial effects of the porous medium and allow for variable ambient temperature. In
                           addition, the applied magnetic field was assumed to be an increasing function of the
                           distancealongtheplate. Prandtlnumberofunitywasassumedinthatstudy. Theresults
                           showed that as the Hartmann number increases, both the skin-friction coefficient and
                           the local Nusselt number are increased. The radiation effect of an optically dense
                           viscous incompressible fluid along a heated inclined flat surface maintained at a
                           uniform temperature and embedded in porous media was studied numerically by
                           Hossain and Pop (1997). The results of that study showed that as the buoyancy
                           parameter increases, the local Nusselt number increases.


                           10.5  NATURAL CONVECTION IN A VERTICAL CHANNEL
                           Analytical solutions for fully developed MHD natural convection flow in open-ended
                           vertical porous channels were presented by Al-Nimr and Hader (1999) using a Darcy
                           model. Four fundamental boundary conditions have been investigated and the cor-
                           responding fundamental solutions were obtained. Expressions for the flow and heat
                           transfer parameters were given in terms of the Darcy number, Prandtl number and
                           other parameters.
                             Transient natural convection between two vertical walls filled with a porous mate-
                           rial having variable porosity was analyzed numerically by Paul et al. (2001) in which
                           inertial and variable porosity effects were investigated. The Brinkman-Forchheimer-
                           extended Darcy model was used to simulate the momentum transfer in the porous
                           domain. A numerical scheme for the transient solution of the governing equations
                           was devised to investigate the channeling effect on the velocity field due to variable
                           porosity of the porous matrix. The finer grid points taken near the walls revealed that
                           the influence of variable porosity is significant only near the heated wall. It was found
                           that the Darcy model predicts an enhancement in the air velocity near the heated wall
                           compared to the general flow model. Formation of the boundary layer near the heated
                           wall was the result of the Brinkman term and its effect was strongly dependent on the
                           diameter of the spherical beads.

                           10.6  NATURAL CONVECTION ABOUT CYLINDERS

                           The local nonsimilarity solution method was applied by Minkowycz and Sparrow
                           (1974) to solve for natural convection on a vertical cylinder for conditions where there
                           were large deviations from the flat plate results. To assess and insure the accuracy
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