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Drag coefficient fluid-solid system

As has already been reported, the case of solid particles can be treated with a simpler approach than that for fluid-fluid systems. One of the most popular correlations for the calculation of the drag coefficient for solid particles suspended in a fluid is that proposed by Wen Yu (1966) ... [Pg.168]

FIG. 17-2 Schematic phase diagram in the region of upward gas flow. W = mass flow solids, lh/(h fr) E = fraction voids Pp = particle density, Ih/ft Py= fluid density, Ih/ft Cd = drag coefficient Re = modified Reynolds uum-her. (Zenz and Othmei Fluidization and Fluid Particle Systems, Reinhold, New York, 1960. )... [Pg.1561]

This result can also be applied directly to coarse particle swarms. For fine particle systems, the suspending fluid properties are assumed to be modified by the fines in suspension, which necessitates modifying the fluid properties in the definitions of the Reynolds and Archimedes numbers accordingly. Furthermore, because the particle drag is a direct function of the local relative velocity between the fluid and the solid (the interstitial relative velocity, Fr), it is this velocity that must be used in the drag equations (e.g., the modified Dallavalle equation). Since Vr = Vs/(1 — Reynolds number and drag coefficient for the suspension (e.g., the particle swarm ) are (after Barnea and Mizrahi, 1973) ... [Pg.429]


See other pages where Drag coefficient fluid-solid system is mentioned: [Pg.168]    [Pg.129]    [Pg.88]    [Pg.88]    [Pg.129]    [Pg.165]    [Pg.165]    [Pg.166]    [Pg.113]    [Pg.132]    [Pg.12]    [Pg.710]    [Pg.27]    [Pg.27]    [Pg.585]   
See also in sourсe #XX -- [ Pg.168 , Pg.169 ]




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