Surfactant and dilatational viscosity effects on the deformation of liquid droplets in an electric field

被引:12
作者
Han, Yu [1 ,2 ]
Koplik, Joel [1 ,3 ]
Maldarelli, Charles [1 ,2 ]
机构
[1] CUNY City Coll, Levich Inst, New York, NY 10031 USA
[2] CUNY City Coll, Dept Chem Engn, New York, NY 10031 USA
[3] CUNY City Coll, Dept Phys, New York, NY 10031 USA
基金
美国国家科学基金会;
关键词
Droplet Deformation; Electrocoalescence; Surfactant; Surface Dilatational Viscosity; Asphaltenes; Langmuir isotherm; CONDUCTING DROP; VISCOUS-FLUID; ELECTROHYDRODYNAMICS; BREAKUP; BURST; ASPHALTENES; STABILITY; SHEAR; ELECTROSPRAY; IONIZATION;
D O I
10.1016/j.jcis.2021.07.105
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Hypothesis: A conducting droplet suspended in an insulating continuous phase, e.g. an aqueous electrolyte in an oil, is deformed by an applied electric field to nonspherical equilibrium shapes, and can even break-up under strong fields. Many technologies use electro-deformation to manipulate fluid dispersions, with surfactants present on the droplet interfaces forming stabilizing monolayers. While surfactants lower the interface tension which facilitates electro-deformation, the monolayer elasticity resists deformation. High molecular weight surfactants, with large dilatational viscosities, can potentially retard the deformation dynamics. Numerics: A boundary integral method simulates the dynamic interfacial deformation of a perfectly conducting droplet in a dielectric in a uniform field. The interface contains an insoluble monolayer which is a Newtonian fluid with constant dilatational viscosity obeying a Langmuir state equation. A range of initial surfactant surface concentrations are studied, with elasticity proportional to concentration. Findings: Equilibrium drop deformations, unaffected by surface viscosity, are strongly resisted by elasticity at high surface concentrations, and field strengths necessary for break-up increase with elasticity. Dilatational viscosity scales with the ratio, kappa*, the surface viscosity (divided by the droplet radius) to the bulk viscosity, and can extend the deformation time. Extended times are described by a time rescaling proportional to kappa*. (C) 2021 Elsevier Inc. All rights reserved.
引用
收藏
页码:900 / 911
页数:12
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