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Mass transport across a flowing gas

Transport across tire direction of flow can be determined using Pick s hrst law of diffusion for dre flux of material in particles/cm sec in a steady, time-independent state [Pg.103]

For a gas in laminar flow over a condensed phase sample of length L, the mass transport across the boundary layer, in terms of the flux of molecules from the sample to die gas phase, is therefore [Pg.104]

The mass transport coefficient in tlris example can be related to the properties of the flowing gas by the equation [Pg.105]

The dimensionless numbers in tlris equation are the Reynolds, Schmidt and the Sherwood number, A/ sh. which is defined by this equation. Dy/g is the diffusion coefficient of the metal-transporting vapour species in the flowing gas. The Reynolds and Schmidt numbers are defined by tire equations [Pg.105]

The advantage of the use of dimensionless numbers in calculations such as these is that they may be applied independent of the physical size of the system being described. [Pg.105]


See other pages where Mass transport across a flowing gas is mentioned: [Pg.103]    [Pg.103]   


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