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Rotating Disk and a Flat Plate

Rotating disk. The mass exchange between a thin rotating disk and the surrounding fluid is governed by Eq. (3.2.1), the boundary conditions at infinity (3.2.2), and a boundary condition at the disk surface of the form (5.1.2) which determines the kinetics of the reaction. It is assumed that the dimensionless concentration is introduced in the same manner as in Subsection 5.1-1. The velocity field of the fluid near a disk is presented in Subsection 1.2-1. [Pg.218]

The solution of this problem shows that relation (5.1.5) is exact in this case for arbitrary kinetics of the surface chemical reaction for any Peclet numbers [270], [Pg.218]

Flat plate. Let us investigate convective diffusion to the surface of a flat plate in a longitudinal translational flow of a viscous incompressible fluid at high Reynolds numbers. The velocity field of the fluid near a flat plate is presented in Subsection 1.7-2. We assume that mass transfer is accompanied by a surface reaction. [Pg.218]

Concentration distribution is described by the steady-state equation (3.1.1) and boundary conditions (3.1.2) and (3.1.5), where = Y is the distance from plate surface. In the diffusion boundary layer approximation, the exact analytical [Pg.218]

In the case of the first-order reaction, the power-series expansion [81] [Pg.219]


Diffusion to a Rotating Disk and a Flat Plate Complicated by a Volume Reaction... [Pg.220]


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