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Sherwood number solid-liquid interface

The dimensionless tangential velocity gradient at the solid-liquid interface, averaged over the front hemisphere of the solid, exhibits a significant influence on the scaling law between the Sherwood and Reynolds nnmbers. Since g (9) is calculated from an analysis of the fluid dynamics problem, it is not a function of the Schmidt number. Hence,... [Pg.301]

For laminar flow adjacent to a high-shear no-slip solid-liquid interface, with one-dimensional flow in the mass transfer boundary layer, the mass transfer coefficient fcA.MXc is obtained from the following Sherwood number correlation (see steps 17 and 18 of Problem 23-7 an page 653, particularly the scaling law exponents a and b) ... [Pg.856]

Figure 4.34. Sherwood number ShL2 required for a minimal liquid-phase transport limitation at L S interface 61 2) a function of substrate concentration with varied values of solid-phase transport limitation represented by which is proportional to particle diameter. The limiting ShL2 number (ShL2 = 2) is indicated. Figure 4.34. Sherwood number ShL2 required for a minimal liquid-phase transport limitation at L S interface 61 2) a function of substrate concentration with varied values of solid-phase transport limitation represented by which is proportional to particle diameter. The limiting ShL2 number (ShL2 = 2) is indicated.

See other pages where Sherwood number solid-liquid interface is mentioned: [Pg.274]    [Pg.301]    [Pg.374]    [Pg.753]    [Pg.284]    [Pg.108]   
See also in sourсe #XX -- [ Pg.301 , Pg.302 , Pg.351 , Pg.355 , Pg.361 , Pg.367 , Pg.653 , Pg.834 ]




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Sherwood number

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Solid-liquid interface

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