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Time-periodic weak solutions for the interaction of an incompressible fluid with a linear Koiter type shell under dynamic pressure boundary conditions

Claudiu Mîndrilă, Sebastian Schwarzacher

Abstract

In many occurrences of fluid-structure interaction time-periodic motions are observed. We consider the interaction between a fluid driven by the three dimensional Navier-Stokes equation and a two dimensional linearized elastic Koiter shell situated at the boundary. The fluid-domain is a part of the solution and as such changing in time periodically. On a steady part of the boundary we allow for the physically relevant case of dynamic pressure boundary values, prominent to model inflow/outflow. We provide the existence of at least one weak time-periodic solution for given periodic external forces that are not too large. For that we introduce new approximation techniques and a-priori estimates.

Time-periodic weak solutions for the interaction of an incompressible fluid with a linear Koiter type shell under dynamic pressure boundary conditions

Abstract

In many occurrences of fluid-structure interaction time-periodic motions are observed. We consider the interaction between a fluid driven by the three dimensional Navier-Stokes equation and a two dimensional linearized elastic Koiter shell situated at the boundary. The fluid-domain is a part of the solution and as such changing in time periodically. On a steady part of the boundary we allow for the physically relevant case of dynamic pressure boundary values, prominent to model inflow/outflow. We provide the existence of at least one weak time-periodic solution for given periodic external forces that are not too large. For that we introduce new approximation techniques and a-priori estimates.
Paper Structure (21 sections, 12 theorems, 159 equations, 1 figure)

This paper contains 21 sections, 12 theorems, 159 equations, 1 figure.

Key Result

Theorem 1.16

Let $\Omega$ be a given reference domain with properties described as above. Then there exists a constant $\tilde{C}$ depending on $\Gamma_p,\Gamma_D,\kappa,L,|M|$ and $c_0$ such that if $\left(\mathbf{f},g,P\right)\in L_{\text{per}}^{2}\left(I;L^2(\mathbb{R}^{3})\right)\times L_{\text{per}}^{2}\lef then there exists at least one weak time-periodic solution $\left(\mathbf{u},\eta\right)$ as it is

Figures (1)

  • Figure 1: The domain $\Omega_{\eta(t)}$

Theorems & Definitions (25)

  • Theorem 1.16
  • Remark 1.20: On the size of $\tilde{C}$ and C
  • Remark 1.21: On the size of $\tilde{C}$ and C
  • Remark 1.22: Case $\Gamma_p=0$
  • Remark 1.23
  • Theorem 1.24
  • Lemma 2.2: Trace operator
  • proof
  • Theorem 2.3
  • Theorem 2.7: Kakutani-Glicksberg-Fan
  • ...and 15 more