Global strong solutions and decay to the 3D full compressible Navier–Stokes equations without heat conductivity

This paper is concerned with the 3D full compressible Naiver-Stokes equations without heat conductivity in bounded domains. For the case when the velocity admits slip boundary condition, global existence and decay rate of strong solutions are established by making full use of the estimate of the gradient of pressure. Compared to previous results in $ H^s $ framework, we only need the initial velocity and pressure to be small in some sense, which indicates that the initial density can contain large oscillations. Moreover, the exponential decay rate of the velocity and pressure are obtained. It should be emphasized that the $ L^2 $–norms of $ {\rm curl} u $ and $ {\rm div}u $ are estimated separately, which shows that $ {\rm curl} u $ decays slower than $ {\rm div}u $ in $ L^2 $ under the condition that the diameter of the domain is suitably large.

Authors

Publication Details

Journal
Discrete and Continuous Dynamical Systems
Published
2024-11-22
DOI
https://doi.org/10.3934/dcds.2024152
Citations
3
Primary Topic
Navier-Stokes equation solutions
Type
article
Field-Weighted Citation Impact
2.93
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article

Global strong solutions and decay to the 3D full compressible Navier–Stokes equations without heat conductivity

Haibo Yu
3 citations
Discrete and Continuous Dynamical Systems
Navier-Stokes equation solutions
2.93
article

Global strong solutions and decay to the 3D full compressible Navier–Stokes equations without heat conductivity

Haibo Yu
article en
3 citations

Abstract

This paper is concerned with the 3D full compressible Naiver-Stokes equations without heat conductivity in bounded domains. For the case when the velocity admits slip boundary condition, global existence and decay rate of strong solutions are established by making full use of the estimate of the gradient of pressure. Compared to previous results in $ H^s $ framework, we only need the initial velocity and pressure to be small in some sense, which indicates that the initial density can contain large oscillations. Moreover, the exponential decay rate of the velocity and pressure are obtained. It should be emphasized that the $ L^2 $–norms of $ {\rm curl} u $ and $ {\rm div}u $ are estimated separately, which shows that $ {\rm curl} u $ decays slower than $ {\rm div}u $ in $ L^2 $ under the condition that the diameter of the domain is suitably large.

Discrete and Continuous Dynamical SystemsVol. 45(6)
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Navier-Stokes equation solutions
2.93
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