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Continuous concentration, assuming that all resistance to mass transfer to/from the pellet is within the pellet and no resistance to pellet-fluid mass transfer is on the bulk fluid side. The concentration in the fluid will thus be equal to that in the pellet pore just at the pellet surface: cpe,i = ci. This constraint also automatically ensures flux continuity between the internal pellet domain and the free fluid domain through so-called reaction forces in the finite element formulation.
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Film resistance (mass flux): The flux of mass across the pellet-fluid interface into the pellet is assumed to be rate determined on the bulk fluid side, by film resistance. The resistance is expressed in terms of a film mass transfer coefficient, hD,i, such that the inward flux is
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Mass transfer parameters with Automatic selected. Specify one of the models from the Sherwood number expression list to compute the Sherwood number. There are three models available: Frössling, Rosner, and Garner and Keey. The Frössling equation is the default and probably the most commonly used for packed spheres. All of these are based on the dimensionless Reynolds (Re) and Schmidt (Sc) numbers, which are computed from Density and Dynamic viscosity. Both of these two properties are specified in the Fluid node under the Packed Bed feature.
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Mass transfer parameters with User defined selected. Specify the type of Parameter — Mass transfer coefficient (the default), or Sherwood number, and enter the selected quantity in the corresponding edit field.
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