Abstract

We study numerically the nonlinear stationary states of a droplet covered with an insoluble surfactant in a uniaxial extensional flow. We calculate both the eigenfunctions to reveal the instability mechanism and the time-dependent states resulting from it, which provides a coherent picture of the phenomenon. The transition is of the saddle-node type, both with and without surfactant. The flow becomes unstable under stationary linear perturbations. Surfactant considerably reduces the interval of stable capillary numbers. Inertia increases the droplet deformation and decreases the critical capillary number. In the presence of the surfactant monolayer, neither the droplet deformation nor the stability is significantly affected by the droplet viscosity. The transient state resulting from instability is fundamentally different for drops with and without surfactant. Tip streaming occurs only in the presence of surfactants. The critical eigenmode leading to tip streaming is qualitatively the same as that yielding the central pinching mode for a clean interface, which indicates that the small local scale characterizing tip streaming is set during the nonlinear droplet deformation. The viscous surface stress does not significantly affect the droplet deformation and the critical capillary number. However, the damping rate of the dominant mode considerably decreases for viscous surfactants. Interestingly, shear viscous surface stress considerably alters the tip streaming arising in the supercritical regime, even for very small surface viscosities. The viscous surface stresses alter the balance of normal interfacial stresses and affect the surfactant transport over the stretched interface.

Highlights

  • Our analysis extends that of Vlahovska et al (2005, 2009), who calculated the deformation of a surfactant-covered droplet in an extensional flow up to third order in the capillary number, neglecting the surfactant viscosity

  • We studied numerically the steady deformation and breakup of a droplet covered with an insoluble surfactant in a uniaxial extensional flow, focusing our attention on the role of the surface viscosities in both the subcritical and supercritical regimes

  • We considered the full hydrodynamic model, which comprises arbitrary large droplet deformations, a variation of the interfacial tension over the droplet surface, and both the droplet and outer bath inertia

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Summary

Surfactants and surface viscosity

Complex interfaces are those whose mechanics cannot be described solely in terms of the interfacial tension. It is believed that shear surface viscosity can stabilize foams and emulsions by increasing the drainage time during the coalescence of two bubbles/droplets (Fischer & Erni 2007; Ozan & Jakobsen 2019). This effect is similar to that produced by Marangoni stresses, which may mask the role played by surface viscosity in many experiments. It is worth mentioning that surface viscosity may become relevant because of its contribution to the balance of fluid momentum and its effect on the surfactant distribution over the interface, which determines the capillary pressure profile and Marangoni stress (Ponce-Torres et al 2017, 2020)

Surfactant-free droplets in linear flows
Surfactant-covered droplets in linear flows
Surfactant-covered droplets in linear flows: the surface viscosity
The goal of this paper
Governing equations
Numerical method
Results
Droplet shape and stability
Tip streaming
Tip streaming: influence of surface viscosity
Conclusions
Full Text
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