Thermodynamic potential of a mechanical constitutive model for two-phase band flow

TL;DR

This paper provides a theoretical explanation for the stable stress plateau in highly sheared viscoelastic fluids using a reduced model analysis related to phase transition theory.

Contribution

It introduces a reduction theory for the non-local diffusive Johnson-Segalman model to explain the stable stress plateau phenomenon.

Findings

The stress plateau is explained as a stable state in the model.

Reduction theory links the model to phase transition dynamics.

Provides a rigorous theoretical foundation for observed flow behavior.

Abstract

Starting from a simple mechanical constitutive model (the non-local diffusive Johnson-Segalman model; DJS model), we provide a rigorous theoretical explanation as to why a unique value of the stress plateau of a highly sheared viscoelastic fluid is stably realized. The present analysis is based on a reduction theory of the degrees of freedom of the model equation in the neighborhood of a critical point, which leads to a time-evolution equation that is equivalent to those for first-order phase transitions.