Large time behavior for the 3D Navier-Stokes with Navier boundary conditions

Fuente: arXiv
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Autori principali: Kelliher, James P., Lacave, Christophe, Filho, Milton C. Lopes, Lopes, Helena J. Nussenzveig, Titi, Edriss S.
Natura: Preprint
Pubblicazione: 2023
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author Kelliher, James P.
Lacave, Christophe
Filho, Milton C. Lopes
Lopes, Helena J. Nussenzveig
Titi, Edriss S.
author_facet Kelliher, James P.
Lacave, Christophe
Filho, Milton C. Lopes
Lopes, Helena J. Nussenzveig
Titi, Edriss S.
contents We study the three-dimensional incompressible Navier-Stokes equations in a smooth bounded domain $Ω$ with initial velocity $u_0$ square-integrable, divergence-free and tangent to $\partial Ω$. We supplement the equations with the Navier friction boundary conditions $u \cdot n = 0$ and $[(2Su)n + αu]_{tang} = 0$, where $n$ is the unit exterior normal to $\partial Ω$, $Su = (Du + (Du)^t)/2$, $α\in C^0(\partialΩ)$ is the boundary friction coefficient and $[\cdot]_{tang}$ is the projection of its argument onto the tangent space of $\partial Ω$. We prove global existence of a weak Leray-type solution to the resulting initial-boundary value problem and exponential decay in energy norm of these solutions when friction is positive. We also prove exponential decay if friction is non-negative and the domain is not a solid of revolution. These two results are well known in the case of Dirichlet boundary condition, but, even if they have been implicitly used for the Navier boundary conditions, the comprehensive analysis is not available in the literature. After carefully studying the Stokes semigroup for such a boundary condition, we use the Galerkin method for existence, Poincaré-type inequalities, with suitable adaptations to account for the differential geometry of the boundary, and a novel integral Gronwall-type inequality. In addition, in the frictionless case $α= 0$, we prove convergence of the solution to a steady rigid rotation, if the domain is a solid of revolution.
format Preprint
id arxiv_https___arxiv_org_abs_2303_03489
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Large time behavior for the 3D Navier-Stokes with Navier boundary conditions
Kelliher, James P.
Lacave, Christophe
Filho, Milton C. Lopes
Lopes, Helena J. Nussenzveig
Titi, Edriss S.
Analysis of PDEs
We study the three-dimensional incompressible Navier-Stokes equations in a smooth bounded domain $Ω$ with initial velocity $u_0$ square-integrable, divergence-free and tangent to $\partial Ω$. We supplement the equations with the Navier friction boundary conditions $u \cdot n = 0$ and $[(2Su)n + αu]_{tang} = 0$, where $n$ is the unit exterior normal to $\partial Ω$, $Su = (Du + (Du)^t)/2$, $α\in C^0(\partialΩ)$ is the boundary friction coefficient and $[\cdot]_{tang}$ is the projection of its argument onto the tangent space of $\partial Ω$. We prove global existence of a weak Leray-type solution to the resulting initial-boundary value problem and exponential decay in energy norm of these solutions when friction is positive. We also prove exponential decay if friction is non-negative and the domain is not a solid of revolution. These two results are well known in the case of Dirichlet boundary condition, but, even if they have been implicitly used for the Navier boundary conditions, the comprehensive analysis is not available in the literature. After carefully studying the Stokes semigroup for such a boundary condition, we use the Galerkin method for existence, Poincaré-type inequalities, with suitable adaptations to account for the differential geometry of the boundary, and a novel integral Gronwall-type inequality. In addition, in the frictionless case $α= 0$, we prove convergence of the solution to a steady rigid rotation, if the domain is a solid of revolution.
title Large time behavior for the 3D Navier-Stokes with Navier boundary conditions
topic Analysis of PDEs
url https://arxiv.org/abs/2303.03489