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Particle nonisotropic

Mean Velocity of Nonisotropic Particles Falling in a Fluid... [Pg.86]

An evaluation of the retardation effects of surfactants on the steady velocity of a single drop (or bubble) under the influence of gravity has been made by Levich (L3) and extended recently by Newman (Nl). A further generalization to the domain of flow around an ensemble of many drops or bubbles in the presence of surfactants has been completed most recently by Waslo and Gal-Or (Wl). The terminal velocity of the ensemble is expressed in terms of the dispersed-phase holdup fraction and reduces to Levich s solution for a single particle when approaches zero. The basic theoretical principles governing these retardation effects will be demonstrated here for the case of a single drop or bubble. Thermodynamically, this is a case where coupling effects between the diffusion of surfactants (first-order tensorial transfer) and viscous flow (second-order tensorial transfer) takes place. Subject to the Curie principle, it demonstrates that this retardation effect occurs on a nonisotropic interface. Therefore, it is necessary to express the concentration of surfactants T, as it varies from point to point on the interface, in terms of the coordinates of the interface, i.e.,... [Pg.329]

To evaluate the volume integrals in (84), the radial distribution function must be known. The pair distribution function affected by the Brownian motion and the relative electrophoretic velocity between a pair of particles is generally nonuniform and nonisotropic. When the particles are sufficiently small so that Brownian motion dominates, one can use a simple distribution function based on hard-sphere potential... [Pg.622]


See other pages where Particle nonisotropic is mentioned: [Pg.25]    [Pg.25]    [Pg.85]    [Pg.162]    [Pg.25]    [Pg.25]    [Pg.85]    [Pg.162]    [Pg.643]    [Pg.411]    [Pg.146]    [Pg.623]    [Pg.203]    [Pg.56]    [Pg.58]    [Pg.187]   
See also in sourсe #XX -- [ Pg.85 , Pg.86 ]




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