<p>The asymptotic analysis of two-dimensional Oldroyd fluid flow equations for viscoelastic fluids in a bounded domain <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\Omega \)</EquationSource> </InlineEquation> with a <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\textrm{C}^2\)</EquationSource> </InlineEquation>-boundary <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\partial \Omega ,\)</EquationSource> </InlineEquation> is carried out in this work. If the forcing term <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\varvec{f}\)</EquationSource> </InlineEquation> is in the space <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbb {L}^2(\Omega )\)</EquationSource> </InlineEquation>, then we show that the global attractor for 2D Oldroyd system is compact not only in the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mathbb {L}^2\)</EquationSource> </InlineEquation>-norm but also in the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {H}^1\)</EquationSource> </InlineEquation>-norm whenever the divergence-free initial data is in <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathbb {H}^1_{0}(\Omega )\)</EquationSource> </InlineEquation>. The existence of an absorbing set and flattening property of the semigroup associated with the concerned system are exploited in the proofs.</p>

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The \(\mathbb {H}^1\)-compact global attractor for the two-dimensional Oldroyd fluid flow equations in bounded domains

  • Kush Kinra,
  • Manil T. Mohan

摘要

The asymptotic analysis of two-dimensional Oldroyd fluid flow equations for viscoelastic fluids in a bounded domain \(\Omega \) with a \(\textrm{C}^2\) -boundary \(\partial \Omega ,\) is carried out in this work. If the forcing term \(\varvec{f}\) is in the space \(\mathbb {L}^2(\Omega )\) , then we show that the global attractor for 2D Oldroyd system is compact not only in the \(\mathbb {L}^2\) -norm but also in the \(\mathbb {H}^1\) -norm whenever the divergence-free initial data is in \(\mathbb {H}^1_{0}(\Omega )\) . The existence of an absorbing set and flattening property of the semigroup associated with the concerned system are exploited in the proofs.