Abstract

The air–water interface in flowing systems remains a challenge to model, even in cases where the interface is essentially flat. This is because even though each side is governed by the Navier–Stokes equations, the stress balance which provides the boundary conditions for the equations involves properties associated with surfactants that are inevitably present at the air–water interface. Aside from challenges in measuring interfacial properties, either intrinsic or flow-dependent, the two-way coupling of bulk and interfacial flows is non-trivial, even for very simple flow geometries. Here, we present an overview of the physics associated with surfactant monolayers of flowing liquid and describe how the monolayer affects the bulk flow and how the monolayer is transported and deformed by the bulk flow. The emphasis is primarily on cylindrical flow geometries, and both Newtonian and non-Newtonian interfacial responses are considered. We consider interfacial flows that are solenoidal as well as those where the surface velocity is not divergence free.

Highlights

  • We provide an overview of the hydrodynamics associated with surfactants, due to their omnipresence in both natural and manmade systems

  • Here we present the theoretical foundation for two-way coupling of inertial bulk flow with surfactant-covered interfaces

  • In purely shearing interfacial flows, many simple monomolecular films exhibit a Newtonian response under varying flow conditions and different flow geometries, yielding a consistent measurement of their surface shear viscosity [18,47]

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Summary

Interfacial Stress Balance

The coupling between the interfacial and bulk flows occurs because of a stress balance. In purely shearing interfacial flows (with no interfacial dilation or compression), many simple monomolecular films exhibit a Newtonian response under varying flow conditions and different flow geometries, yielding a consistent measurement of their surface shear viscosity [18,47]. These interfaces exhibit well-understood Marangoni stresses [17,48]. Numerical simulations of the flow in the ring-sheared drop, presented in Figure 2b,c, illustrate the effects of the surface shear viscosity on the vortex lines.

Modeling the Non–Newtonian Interfacial Response
Two-Way Coupled Flows
Marangoni Effects
A A ΩA AAAAAAAA
Surface Dilatational Viscosity and Non-Equilibrium Monolayer State
Conclusions
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