Abstract

Within this work, we upscale the equations that describe the pore-scale behaviour of nonlinear porous elastic composites, using the asymptotic homogenization technique in order to derive the macroscale effective governing equations. A porous hyperelastic composite can be thought of as being comprised of a matrix interacting with a number of subphases and percolated by a fluid flowing in the pores (which is chosen to be Newtonian and incompressible here). A general nonlinear macroscale model is derived and is then specified for a particular choice of strain energy function, namely the de Saint-Venant function. This leads to a macroscale system of PDEs, which is of poroelastic type with additional terms and transformations to account for the nonlinear behaviour of the material. Our new porohyperelastic-type model describes the effective behaviour of nonlinear porous composites by prescribing the stress balance equations, the conservation of mass and Darcy’s law. The coefficients of these macroscale equations encode the detailed microstructure of the material and are to be found by solving pore-scale differential problems. The model reduces to the following limit cases of (a) linear poroelastic composites when the deformation gradient approaches the identity, (b) nonlinear composites when there are no pores and (c) nonlinear poroelasticity when only the matrix–fluid interaction is considered. This model is applicable when the interactions between various hyperelastic solid phases occur at the pore-scale, as in biological tissues such as artery walls, the myocardium, lungs and liver.

Highlights

  • The theory of poroelasticity can be used to describe the effective mechanical behaviour of porous elastic materials with fluid flowing in the pores

  • We set up our fluid–structure interaction with the assumption that all elastic phases are in contact with each other and the fluid

  • We apply a coordinate transformation to the equations in the fluid–structure interaction (FSI) in order to obtain a full system of partial differential equations (PDEs) that describe the structure in the reference configuration

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Summary

Introduction

The theory of poroelasticity can be used to describe the effective mechanical behaviour of porous elastic materials with fluid flowing in the pores. This type of structure can be described as a poroelastic composite material that undergoes large deformations This is applicable to artery walls, which can be considered as a composite nonlinear elastic material consisting of a matrix with two families of symmetrically arranged embedded collagen and elastin fibres as well as fibroblast cells that interact with the fluid that is flowing in the pores [12,34,35,36,37]. We generalise [27] to account for nonlinear deformations by using the asymptotic homogenization technique to upscale the interaction between a hyperelastic porous matrix where there is an incompressible Newtonian fluid flowing in the pores and a number of embedded hyperelastic subphases.

Formulation of the Fluid–Structure Interaction Problem
Fluid–Structure Interaction in Lagrangian Coordinates
The Asymptotic Homogenization Method
Nondimensionalisation
The Two-Scale Asymptotic Homogenization Method
The Macroscale Results
The Macroscale Fluid Flow
The Macroscale Poroelastic Relationships
The Macroscale Model and Particular Cases
Constitutive Law
Comparison with Linear Poroelastic Composites
Comparison with Nonlinear Poroelasticity
Comparison with Nonlinear Elastic Composites
Concluding Remarks
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