Monolithic Framework to Simulate Fluid‐Structure Interaction Problems Using Geometric Volume‐of‐Fluid Method

ABSTRACT We develop a three‐dimensional Eulerian framework to simulate fluid‐structure interaction (FSI) problems on a fixed Cartesian grid using the geometric volume‐of‐fluid (VOF) method. The coupled problem involves incompressible flow and viscous hyperelastic solids. A VOF‐based one‐continuum formulation is used to describe the unified momentum conservation equations with incompressibility constraints that are solved using the finite volume method (FVM). In the geometric VOF interface‐capturing (IC) approach, the piecewise linear interface calculation (PLIC) method is used to reconstruct the interface, and the Lagrangian explicit (LE) method is used in the directionally split advection procedure. To model the hyperelastic behavior of the solid, we consider linear and nonlinear Mooney–Rivlin material models, where we use the left Cauchy–Green deformation tensor () to account for the solid deformation on an Eulerian grid and the fifth‐order weighted essentially non‐oscillatory (WENO‐Z) finite difference reconstruction method is utilized to treat the advection terms involved in the transport equation of . Multiple benchmark problems and reversibility tests are considered to verify the accuracy of the approach. Furthermore, to demonstrate the capability of the solver to handle turbulent interactions, we perform direct numerical simulation (DNS) of turbulent channel flow with a deformable compliant bottom wall and a rigid top wall; our observations align well with previous experimental and numerical works. The detailed numerical experiments show that: (i) despite the discontinuity of the interface across the cell boundaries and stress discontinuity across the interface, a VOF/PLIC‐based FSI framework can provide stable and accurate solutions that significantly minimizes numerical artifacts (e.g., flotsam and spurious currents) while maintaining a sharp interface. (ii) The accuracy of a VOF/PLIC‐based FSI approach on coarse grids is comparable to the accuracy of a diffusive IC method‐based FSI approach on much finer grids.