Abstract

A framework is presented for the formulation of a class of continuum constitutive models for sharp interfaces with non-linear viscoelastic behaviour due to a considerable isotropic interfacial microstructure. For the formulation of a thermodynamically consistent elastoviscoplastic interface constitutive model we adapt an approach successful in describing the behaviour of bulk polymer glasses. The model has a clear separation between dilatation and shear, and is used to predict phenomena related to the plasticity of interfaces observed in the experimental literature, which is relevant for many applications. Stress–strain predictions in standard interfacial rheological flows, i.e. shear and dilatation, are investigated numerically. A predominantly elastic response is obtained at small deformations, with a transition to primarily plastic flow at high stress levels. In interfacial shear flow, strain softening and eventually a plastic plateau occur upon further deformation beyond the yield point. The yield stress and strain and (the relative strength of) the stress overshoot in interfacial shear flow are shown to be controlled by two dimensionless groups of parameters in the model. In interfacial dilatation, the model predicts elastoviscoplastic behaviour with a stress maximum and a decreasing stress without a plateau at even larger deformations. These phenomena are studied for various choices for the parameters in the model. • Framework for non-linear viscoelastic interface models is developed. • Thermodynamic consistency is intrinsically respected in the framework. • Existing viscoelastic interface models are reviewed. • New elastoviscoplastic interface model is proposed. • Qualitative agreement with experiments in both shear and dilatation is found.

Highlights

  • Plastic behaviour of fluid-fluid interfaces in foams and emulsions is relevant in many applications such as foods, consumer products, pharmaceuticals, petrochemicals, polymer technology, and in nature and biology

  • In addition to the interfacial Upper-Convected Maxwell (UCM) and Lower-Convected Maxwell (LCM) models presented in Secs. 3.3.1-3.3.2, we have tried to derive the surface upper-convected Maxwell (SUCM) model often encountered in the literature, see [11, 15], starting from a similar Lodge-type integral as for UCM and LCM

  • The model has a clear separation between interfacial dilatation and shear, which is useful for experiments

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Summary

Introduction

Plastic behaviour of fluid-fluid interfaces in foams and emulsions is relevant in many applications such as foods, consumer products, pharmaceuticals (drug delivery), petrochemicals (oil recovery), polymer technology (polymer blends), and in nature and biology. In interfacial large amplitude oscillatory extension and step extensional strain (rate) experiments, similar results as for their interfacial shear experiment counterparts have been obtained [5,6,7]. In contrast to shear experiments, for extension in [5,6,7] 35 no overshoot in the stress was observed during plastic flow When it comes to modelling the non-linear viscoelasticity of interfaces, two approaches are followed in the literature.

Kinematics of interfaces
Curvilinear coordinates
Deformation
Rate of deformation
Constitutive modelling
Viscoelastic models
Lower-convected Maxwell
Surface upper-convected Maxwell model from the literature
Giesekus model
Application to homogeneous flows
Single-point calculations for dilatation
Discussion: comparison with the Eindhoven Glassy Polymer model
Conclusions and recommendations
500 References
Full Text
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