Article | REF: J1065 V1

Elements of fluid mechanics - Application to porous media

Author: Jean-Claude CHARPENTIER

Publication date: September 10, 1999 | Lire en français

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    3. Movement of drops and bubbles

    A fluid globule is distinguished from a rigid spherical globule by its viscosity η g , which is not infinite, and by the continuous globule/phase interfacial tension σ.

    For a spherical globule of diameter d, which is subjected neither to deformation nor oscillation, and in laminar flow (Re g < 1), the globule's velocity is equal to the free-fall velocity given by Stokes' formula (6) , multiplied by a corrective factor, Hadamard's coefficient H :

    H=3η+3ηg2η+3ηg

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