Abstract

The immersed boundary method is an approach to fluid‐structure interaction that uses a Lagrangian description of the structural deformations, stresses, and forces along with an Eulerian description of the momentum, viscosity, and incompressibility of the fluid‐structure system. The original immersed boundary methods described immersed elastic structures using systems of flexible fibers, and even now, most immersed boundary methods still require Lagrangian meshes that are finer than the Eulerian grid. This work introduces a coupling scheme for the immersed boundary method to link the Lagrangian and Eulerian variables that facilitates independent spatial discretizations for the structure and background grid. This approach uses a finite element discretization of the structure while retaining a finite difference scheme for the Eulerian variables. We apply this method to benchmark problems involving elastic, rigid, and actively contracting structures, including an idealized model of the left ventricle of the heart. Our tests include cases in which, for a fixed Eulerian grid spacing, coarser Lagrangian structural meshes yield discretization errors that are as much as several orders of magnitude smaller than errors obtained using finer structural meshes. The Lagrangian‐Eulerian coupling approach developed in this work enables the effective use of these coarse structural meshes with the immersed boundary method. This work also contrasts two different weak forms of the equations, one of which is demonstrated to be more effective for the coarse structural discretizations facilitated by our coupling approach.

Highlights

  • Since its introduction,[1,2] the immersed boundary (IB) method has been widely used to simulate biological fluid dynamics and other problems in which a structure is immersed in a fluid flow.[3]

  • We describe an alternative approach to using finite element (FE) structural discretizations with the IB method that combines a Cartesian grid finite difference method for the incompressible Navier-Stokes equations with a nodal FE method for the structural mechanics

  • For γ = 0, the initial configuration of the shell is a circular annulus with inner radius R and thickness w, which corresponds to an equilibrium configuration of the structure

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Summary

INTRODUCTION

Since its introduction,[1,2] the immersed boundary (IB) method has been widely used to simulate biological fluid dynamics and other problems in which a structure is immersed in a fluid flow.[3]. We apply the present IB method to benchmark fluid-structure interaction (FSI) problems involving elastic, rigid, and actively contracting structures, including an idealized model of the left ventricle of the heart.[45] For elastic structures, we consider two weak formulations of the equations of motion suitable for standard nodal (C0) FE methods for structural mechanics One of these formulations, referred to as the unified weak form, is similar to those used by earlier IB-like methods.[30,31,32,33,34,37,38,39] This formulation uses a single volumetric force density to describe the mechanical response of the immersed structure. The present IB method is the first IFE-type method to explicitly enable the effective use of such relatively coarse Lagrangian meshes

Immersed elastic bodies
Strong formulation
Weak formulations
Immersed rigid structures
Eulerian discretization
Eulerian inner products
Lagrangian discretization
Immersed elastic structures
Lagrangian inner products
Lagrangian-Eulerian interaction
IMPLEMENTATION
Thick elliptical shell
Anisotropic shell
Orthotropic shell
Soft elastic disc in lid driven cavity
Flow past a cylinder
Idealized model of left ventricular mechanics
Passive inflation of an isotropic left ventricle model
Active contraction of a fiber-reinforced left ventricle model
DISCUSSION AND CONCLUSIONS
Basic time-stepping scheme
Initial time step

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