Flow around a droplet suspended in a yield-stress fluid

Author:

Pourzahedi Ali1ORCID,Chaparian Emad2ORCID,Frigaard Ian A.13ORCID

Affiliation:

1. Department of Mechanical Engineering, University of British Columbia 1 , 2054-6250 Applied Science Lane, Vancouver, British Columbia V6T 1Z4, Canada

2. James Weir Fluid Laboratory, Department of Mechanical and Aerospace Engineering, University of Strathclyde 2 , Glasgow G1 1XJ, United Kingdom

3. Department of Mathematics, University of British Columbia 3 , 1984 Mathematics Road, Vancouver, British Columbia V6T 1Z2, Canada

Abstract

We investigate the minimal yield-stress required in order to hold static an ellipsoidal Newtonian droplet inside a yield-stress liquid. This critical limit (Yc) is influenced by the droplet aspect ratio (χ), the interfacial tension (γ), and the viscosity ratio (M) between the droplet and the surrounding liquid, as well as the ratio of the yield-stress to the buoyancy stress (Y). The droplet will remain trapped by the liquid yield-stress for Y>Yc. Our study bridges the gap in the published results between those calculated for bubbles (M→0) and the solid rigid particles (M→∞), being of practical use for those estimating the design of stable yield-stress emulsions. In general, the critical yield number increases with the interfacial tension and the droplet aspect ratio and will decrease with the droplet viscosity. For spherical droplets, our results computed for yield numbers below Yc suggest that the spherical shaped droplet may propagate in steady motion.

Funder

NSERC

Publisher

AIP Publishing

Reference42 articles.

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4. Stokes paradox for power-law flow around a cylinder;J. Non-Newtonian Fluid Mech.,1993

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