Friedrich-Alexander University Erlangen-Nürnberg, Department of Mathematics, Cauerstraße 11, 91058 Erlangen, Germany.
Rice University, Department of Computational and Applied Mathematics, 6100 Main Street, Houston, TX 77005, USA.
J Colloid Interface Sci. 2018 Aug 1;523:282-291. doi: 10.1016/j.jcis.2018.02.075. Epub 2018 Mar 17.
We consider an energy-based boundary condition to impose an equilibrium wetting angle for the Cahn-Hilliard-Navier-Stokes phase-field model on voxel-set-type computational domains. These domains typically stem from μCT (micro computed tomography) imaging of porous rock and approximate a (on μm scale) smooth domain with a certain resolution. Planar surfaces that are perpendicular to the main axes are naturally approximated by a layer of voxels. However, planar surfaces in any other directions and curved surfaces yield a jagged/topologically rough surface approximation by voxels. For the standard Cahn-Hilliard formulation, where the contact angle between the diffuse interface and the domain boundary (fluid-solid interface/wall) is 90°, jagged surfaces have no impact on the contact angle. However, a prescribed contact angle smaller or larger than 90° on jagged voxel surfaces is amplified. As a remedy, we propose the introduction of surface energy correction factors for each fluid-solid voxel face that counterbalance the difference of the voxel-set surface area with the underlying smooth one. The discretization of the model equations is performed with the discontinuous Galerkin method. However, the presented semi-analytical approach of correcting the surface energy is equally applicable to other direct numerical methods such as finite elements, finite volumes, or finite differences, since the correction factors appear in the strong formulation of the model.
我们考虑基于能量的边界条件,为 Cahn-Hilliard-Navier-Stokes 相场模型在体素集型计算域上施加平衡润湿角。这些域通常源自多孔岩石的 μCT(微计算机断层扫描)成像,并以一定的分辨率近似于(在 μm 尺度上)平滑域。垂直于主轴的平面自然由一层体素近似。然而,任何其他方向的平面和曲面通过体素产生锯齿状/拓扑粗糙的表面近似。对于标准的 Cahn-Hilliard 公式,其中扩散界面和域边界(流体-固体界面/壁)之间的接触角为 90°,锯齿状表面对接触角没有影响。然而,在锯齿状体素表面上规定的小于或大于 90°的接触角会被放大。作为一种补救措施,我们提出为每个流体-固体体素面引入表面能修正因子,以平衡体素表面积与基础平滑表面积之间的差异。模型方程的离散化采用不连续 Galerkin 方法。然而,所提出的修正表面能的半解析方法同样适用于其他直接数值方法,如有限元、有限体积或有限差分,因为修正因子出现在模型的强形式中。