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Global existence and Rayleigh-Taylor instability for the semi-dissipative Boussinesq system with Naiver boundary conditions

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arxiv 2405.16074 v1 pith:SJ47V4X5 submitted 2024-05-25 math.DS

classification math.DS
keywords existenceglobalboundaryconditionsinstabilityomegasolutionsdomain
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abstract

Considered herein is the global existence of weak, strong solutions and Rayleigh-Taylor (RT) instability for 2D semi-dissipative Boussinesq equations in an infinite strip domain $\Omega_{\infty}$ subject to Navier boundary conditions with non-positive slip coefficients. We first prove the global existence of weak and strong solutions on bounded domain $\Omega_{R}$ via the Galerkin method, characteristic analyzing technique and Stokes estimates etc. Based on above results, we further derive the uniform estimates, independent of the length of horizontal direction of $\Omega_{R}$, ensuring the global existence of weak and strong solutions in unbounded case $\Omega_{\infty}$ by utilizing the domain expansion method. Moreover, when the steady temperature is higher with decreasing height (i.e., RT steady-state) on certain region, we demonstrate that the steady-state is linear unstable through the construction of energy functional and the settlement of a family of modified variational problems. Furthermore, with the help of unstable solutions constructed in linear instability and global existence theorems, we confirm the instability of nonlinear problem in a Lipschitz structural sense. Finally, we give a series of rigorous verification (see Appendix) including the spectra of Stokes equations with Navier boundary conditions, Sobolev embedding inequalities, trace inequalities, and Stokes estimates under Navier boundary conditions etc, used in the proof of main conclusions.

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  1. Exponential decay for the 3D Boussinesq equations with Navier boundary conditions

    math.AP 2026-08 accept novelty 6.0 of 10

    Exponential decay of energy is established for 3D Boussinesq and Navier-Stokes flows with Navier slip boundary conditions under only localized positive friction, via a new weighted Korn-Poincaré inequality.

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