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Axisymmetric creeping motion of drops through circular tubes

Published online by Cambridge University Press:  26 April 2006

M. J. Martinez
Affiliation:
Department of Mechanical Engineering, University of California at Berkeley, Berkeley, CA 94720, USA Current address: Fluid and Thermal Sciences Department, Sandia National Laboratories, Albuquerque, NM 87185, USA.
K. S. Udell
Affiliation:
Department of Mechanical Engineering, University of California at Berkeley, Berkeley, CA 94720, USA

Abstract

The axisymmetric creeping motion of a neutrally buoyant deformable drop flowing through a circular tube is analysed with a boundary integral equation method. The fluids are immiscible, incompressible, and the bulk flow rate is constant. The drop to suspending fluid viscosity ratio is arbitrary and the drop radius varies from 0.5 to 1.15 tube radii. The effects of the capillary number, viscosity ratio, and drop size on the deformation, the drop speed, and the additional pressure loss are examined.

Drops with radius ratios less than 0.7 are insensitive to substantial variation in capillary number and viscosity ratio, and computed values of drop speed and extra pressure loss are in excellent agreement with small deformation theories (Hestroni et al. 1970; Hyman & Skalak 1972a). For this drop size range, significant deformation will result only for Ca > 0.25. The onset of a re-entrant cavity is predicted at the trailing end of the drop for Ca ≈ 0.75. Drop speed and meniscus shape become independent of drop size for radius ratios as small as 1.10. The extra pressure loss can be positive or negative depending mainly on the viscosity ratio, however a relatively inviscid drop can cause a positive extra pressure loss when capillary forces are significant. Computed values for extra pressure loss and drop speed are in good agreement with the experimental data of Ho & Leal (1975) for drops of sizes comparable with the tube radius.

Type
Research Article
Copyright
© 1990 Cambridge University Press

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