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On a phase field model for binary mixtures of micropolar fluids with non-matched densities and moving contact lines

Kin Shing Chan, Baoli Hao, Kei Fong Lam, Björn Stinner

TL;DR

This work develops a thermodynamically consistent phase-field model for binary mixtures of incompressible micropolar fluids with non-matched densities and moving contact lines. It couples a volume-averaged Navier–Stokes–Cahn–Hilliard system for $(\bm{u}, p, \phi, \mu)$ with a micropolar equation for $\bm{\omega}$, and derives the model from conservation laws under an energy-dissipation framework. The paper presents both local (logarithmic) and nonlocal/free-energy formulations, and establishes global weak solutions in 3D for the singular potentials, including a deep quench limit to the obstacle potential. The analysis adopts a two-stage approximation with implicit time discretisation, yielding robust existence results and laying groundwork for numerical analysis of moving-contact-line two-phase flows in micropolar fluids.

Abstract

We introduce a new phase field model for binary mixtures of incompressible micropolar fluids, which are among the simplest categories of fluids exhibiting internal rotations. The model fulfils local and global dissipation inequalities so that thermodynamic consistency is guaranteed. Our model consists of a Navier--Stokes--Cahn--Hilliard system for the fluid velocity, pressure, phase field variable and chemical potential, coupled to an additional system of Navier--Stokes type for the micro-rotation. Our model accounts for non-matched densities as well as moving contact line dynamics, and serve as a generalisation to earlier models for binary fluid flows based on a volume averaged velocity formulation. We also establish the existence of global weak solutions in three spatial dimensions for the model equipped with singular logarithmic and double obstacle potentials.

On a phase field model for binary mixtures of micropolar fluids with non-matched densities and moving contact lines

TL;DR

This work develops a thermodynamically consistent phase-field model for binary mixtures of incompressible micropolar fluids with non-matched densities and moving contact lines. It couples a volume-averaged Navier–Stokes–Cahn–Hilliard system for with a micropolar equation for , and derives the model from conservation laws under an energy-dissipation framework. The paper presents both local (logarithmic) and nonlocal/free-energy formulations, and establishes global weak solutions in 3D for the singular potentials, including a deep quench limit to the obstacle potential. The analysis adopts a two-stage approximation with implicit time discretisation, yielding robust existence results and laying groundwork for numerical analysis of moving-contact-line two-phase flows in micropolar fluids.

Abstract

We introduce a new phase field model for binary mixtures of incompressible micropolar fluids, which are among the simplest categories of fluids exhibiting internal rotations. The model fulfils local and global dissipation inequalities so that thermodynamic consistency is guaranteed. Our model consists of a Navier--Stokes--Cahn--Hilliard system for the fluid velocity, pressure, phase field variable and chemical potential, coupled to an additional system of Navier--Stokes type for the micro-rotation. Our model accounts for non-matched densities as well as moving contact line dynamics, and serve as a generalisation to earlier models for binary fluid flows based on a volume averaged velocity formulation. We also establish the existence of global weak solutions in three spatial dimensions for the model equipped with singular logarithmic and double obstacle potentials.
Paper Structure (18 sections, 5 theorems, 182 equations)

This paper contains 18 sections, 5 theorems, 182 equations.

Key Result

Theorem 3.1

Under Assumption ass:main, for any $T \in (0,\infty)$ there exists a weak solution to ana:bulk-ana:bc in the sense of Definition defn:weaksoln.

Theorems & Definitions (18)

  • Remark 2.1
  • Remark 2.2
  • Remark 2.3
  • Remark 2.4
  • Remark 2.5: Reformulation of the linear pseudo-momentum balance
  • Remark 2.6: Reformulation of the linear pseudo-momentum balance
  • Definition 3.1
  • Theorem 3.1
  • Definition 3.2
  • Theorem 3.2
  • ...and 8 more