On global existence and large-time behaviour of weak solutions to the compressible barotropic Navier--Stokes Equations on $\mathbb{T}^2$ with density-dependent bulk viscosity: beyond the Va\u{\i}gant--Kazhikhov regime

TL;DR

This paper advances the understanding of weak solutions to the 2D compressible barotropic Navier--Stokes equations with density-dependent viscosity, establishing global existence and large-time behavior under broader conditions than previously known.

Contribution

It proves global existence of weak solutions for a wider parameter range and shows the density remains bounded away from zero and infinity over time, extending prior results significantly.

Findings

Global existence of weak solutions for eta>1 and >1.

Density remains bounded away from zero and infinity over time.

Extension of the theory to the most general setting to date.

Abstract

We are concerned with the compressible barotropic Navier--Stokes equations for a $\gamma$-law gas with density-dependent bulk viscosity coefficient $\lambda=\lambda(\rho)=\rho^\beta$ on the two-dimensional periodic domain $\mathbb{T}^2$. The global existence of weak solutions with initial density bounded away from zero and infinity for $\beta>3$, $\gamma>1$ has been established by Va\u{\i}gant--Kazhikhov [\textit{Sib. Math. J.} 36 (1995), 1283--1316]. When $\gamma=\beta>3$, the large-time behaviour of the weak solutions and, in particular, the absence of formation of vacuum and concentration of density as $t \to \infty$, has been proved by Perepelitsa [\textit{SIAM J. Math. Anal.} 39 (2007/08), 1344--1365]. Huang--Li [\textit{J. Math. Pures Appl.} 106 (2016), 123--154] extended these results by establishing the global existence of weak solutions and large-time behaviour under the assumptions $\beta >3/2$, $1< \gamma<4\beta-3$, and that the initial density stays away from infinity (but may contain vacuum). Improving upon the works listed above, we prove that in the regime of parameters as in Huang--Li, namely that $\beta >3/2$ and $1< \gamma<4\beta-3$, if the density has no vacuum or concentration at $t=0$, then it stays away from zero and infinity at all later time $t \in ]0,\infty[$. Moreover, under the mere assumption that $\beta>1$ and $\gamma>1$, we establish the global existence of weak solutions, thus pushing the global existence theory of the barotropic Navier--Stokes equations on $\mathbb{T}^2$ to the most general setting to date. One of the key ingredients of our proof is a novel application -- motivated by the recent work due to Danchin--Mucha [\textit{Comm. Pure Appl. Math.} 76 (2023), 3437--3492] -- of Desjardins' logarithmic interpolation inequality.