Abstract

We study an unsteady nonlinear fluid–structure interaction problem which is a simplified model to describe blood flow through viscoelastic arteries. We consider a Newtonian incompressible two-dimensional flow described by the Navier–Stokes equations set in an unknown domain depending on the displacement of a structure, which itself satisfies a linear viscoelastic beam equation. The fluid and the structure are fully coupled via interface conditions prescribing the continuity of the velocities at the fluid–structure interface and the action–reaction principle. We prove that strong solutions to this problem are global-in-time. We obtain, in particular that contact between the viscoelastic wall and the bottom of the fluid cavity does not occur in finite time. To our knowledge, this is the first occurrence of a no-contact result, and of the existence of strong solutions globally in time, in the frame of interactions between a viscous fluid and a deformable structure.

Highlights

  • We focus on the interactions between a viscous incompressible Newtonian fluid and a moving viscoelastic structure located on one part of the fluid domain boundary

  • This work is motivated by the study of blood flow in arteries and the fluid-structure interaction (FSI) model we consider here can be viewed as a simplified version of a standard model/benchmark for FSI problems/solvers in hemodynamics [42], [13]

  • Consequenlty, we investigate whether or not collision occurs between the moving boundary and the bottom of the fluid cavity together with the existence of global-in-time strong solutions

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Summary

Introduction

We focus on the interactions between a viscous incompressible Newtonian fluid and a moving viscoelastic structure located on one part of the fluid domain boundary. Our proof for Theorem 1 follows a classical scheme: local-in-time existence and uniqueness of solutions, blow-up alternative and a priori estimates.

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