<p>This article presents an asymptotic analysis of a periodic micropolar fluid flow in an infinite thin channel with an impervious wall and an elastic stratified stiff wall in the context of fluid-structure interaction problems. The considered model was introduced in a previous article (Panasenko et al. in Math. Model. Anal. 29(4):641–668, <CitationRef CitationID="CR1">2024</CitationRef>) and it depends on a small parameter, <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> <EquationSource Format="TEX">${\varepsilon }$</EquationSource> </InlineEquation>, defined as the ratio between the thickness of the elastic structure and that of the fluid layer. We perform an asymptotic analysis with respect to this small parameter for a suitable scaling of the physical data depending on&#xa0;<InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> <EquationSource Format="TEX">${\varepsilon }$</EquationSource> </InlineEquation>. Corresponding to this choice, the densities are of order&#xa0;<InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mn>0</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">${\varepsilon }^{0}$</EquationSource> </InlineEquation>, the elasticity coefficients (the Young’s moduli of the stratified elastic structure) are of order <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mrow> <mo>−</mo> <mn>3</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">${\varepsilon }^{-3}$</EquationSource> </InlineEquation> and the external forces acting on the elastic material are of order&#xa0;<InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <msup> <mi>ε</mi> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">${\varepsilon }^{-1}$</EquationSource> </InlineEquation>. We define an asymptotic solution of order <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <mi>J</mi> </math></EquationSource> <EquationSource Format="TEX">$J$</EquationSource> </InlineEquation> expressed by means of matrix-valued, vectorial and scalar functions and then we construct and solve the problems for these unknown functions. We provide next a rigorous justification of the asymptotic construction. More precisely, we show that the error between the solution of the physical problem and the asymptotic solution of order <InlineEquation ID="IEq7"> <EquationSource Format="MATHML"><math> <mi>J</mi> </math></EquationSource> <EquationSource Format="TEX">$J$</EquationSource> </InlineEquation> with respect to suitable norms is of order <InlineEquation ID="IEq8"> <EquationSource Format="MATHML"><math> <mi mathvariant="script">O</mi> <mo stretchy="false">(</mo> <msup> <mi>ε</mi> <mrow> <mi>J</mi> <mo>+</mo> <mi>υ</mi> </mrow> </msup> <mo stretchy="false">)</mo> </math></EquationSource> <EquationSource Format="TEX">${\mathcal{O}}({\varepsilon }^{J+\upsilon })$</EquationSource> </InlineEquation> for any <InlineEquation ID="IEq9"> <EquationSource Format="MATHML"><math> <mi>J</mi> <mo>≥</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$J \ge 0$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq10"> <EquationSource Format="MATHML"><math> <mi>υ</mi> </math></EquationSource> <EquationSource Format="TEX">$\upsilon $</EquationSource> </InlineEquation> a positive fixed number. This means that the asymptotic solution of order <InlineEquation ID="IEq11"> <EquationSource Format="MATHML"><math> <mi>J</mi> </math></EquationSource> <EquationSource Format="TEX">$J$</EquationSource> </InlineEquation> represents a good approximation of the exact solution even for <InlineEquation ID="IEq12"> <EquationSource Format="MATHML"><math> <mi>J</mi> <mo>=</mo> <mn>0</mn> </math></EquationSource> <EquationSource Format="TEX">$J=0$</EquationSource> </InlineEquation>, that fully justifies our asymptotic construction.</p>

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Micropolar Fluid-Thin Elastic Structure Interaction: Asymptotic Analysis

  • Grigory P. Panasenko,
  • Laetitia Paoli,
  • Ruxandra Stavre

摘要

This article presents an asymptotic analysis of a periodic micropolar fluid flow in an infinite thin channel with an impervious wall and an elastic stratified stiff wall in the context of fluid-structure interaction problems. The considered model was introduced in a previous article (Panasenko et al. in Math. Model. Anal. 29(4):641–668, 2024) and it depends on a small parameter, ε ${\varepsilon }$ , defined as the ratio between the thickness of the elastic structure and that of the fluid layer. We perform an asymptotic analysis with respect to this small parameter for a suitable scaling of the physical data depending on  ε ${\varepsilon }$ . Corresponding to this choice, the densities are of order  ε 0 ${\varepsilon }^{0}$ , the elasticity coefficients (the Young’s moduli of the stratified elastic structure) are of order ε 3 ${\varepsilon }^{-3}$ and the external forces acting on the elastic material are of order  ε 1 ${\varepsilon }^{-1}$ . We define an asymptotic solution of order J $J$ expressed by means of matrix-valued, vectorial and scalar functions and then we construct and solve the problems for these unknown functions. We provide next a rigorous justification of the asymptotic construction. More precisely, we show that the error between the solution of the physical problem and the asymptotic solution of order J $J$ with respect to suitable norms is of order O ( ε J + υ ) ${\mathcal{O}}({\varepsilon }^{J+\upsilon })$ for any J 0 $J \ge 0$ and υ $\upsilon $ a positive fixed number. This means that the asymptotic solution of order J $J$ represents a good approximation of the exact solution even for J = 0 $J=0$ , that fully justifies our asymptotic construction.