A novel diffuse-interface model and a fully-discrete maximum-principle-preserving energy-stable method for two-phase flow with surface tension and non-matching densities

Journal Article (2021)
Author(s)

M. F.P.ten Eikelder (TU Delft - Ship Hydromechanics and Structures)

I. Akkerman (TU Delft - Ship Hydromechanics and Structures)

Research Group
Ship Hydromechanics and Structures
Copyright
© 2021 M.F.P. ten Eikelder, I. Akkerman
DOI related publication
https://doi.org/10.1016/j.cma.2021.113751
More Info
expand_more
Publication Year
2021
Language
English
Copyright
© 2021 M.F.P. ten Eikelder, I. Akkerman
Research Group
Ship Hydromechanics and Structures
Volume number
379
Reuse Rights

Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons.

Abstract

Two well-established classes of the interface capturing models are the level-set and phase-field models. Level-set formulations satisfy the maximum principle for the density but are not energy-stable. On the other hand, phase-field models do satisfy the second law of thermodynamics but lack the maximum principle for the density. In this paper we derive a novel model for incompressible immiscible two-phase flow with non-matching densities and surface tension that is both energetically-stable and satisfies the maximum principle for the density. The model finds its place at the intersection of level-set and phase-field models. Its derivation is based on a diffusification of the incompressible two-phase Navier–Stokes equations with non-matching densities and surface tension and involves functional entropy variables. Additionally, we present an associated fully-discrete energy-stable method. Isogeometric analysis is used for the spatial discretization and the temporal-integration is performed with a new time-integration scheme that is a perturbation of the second-order midpoint scheme. The fully-discrete scheme is unconditionally energy-dissipative, pointwise divergence-free and satisfies the maximum principle for the density. Numerical examples in two and three dimensions verify the energetic-stability of the methodology.