Abstract

We investigate global stability and nonvanishing vacuum states of large solutions to the compressible Navier–Stokes equations on the torus , and the main purpose of this work is threefold. First, under the assumption that the density verifies , it is shown that the solutions converge to an equilibrium state exponentially in the -norm. In contrast to previous related works where the density has uniform positive lower and upper bounds, this gives the first stability result for large strong solutions of the three-dimensional compressible Navier–Stokes equations in the presence of vacuum. Second, by employing some new thoughts, we also show that the density converges to its equilibrium state exponentially in the -norm if additionally the initial density satisfies . Finally, we prove that the vacuum state will persist for any time provided that the initial density contains vacuum, which is different from the previous work of [H. L. Li, J. Li, and Z. P. Xin, Comm. Math. Phys., 281 (2008), pp. 401–444], where the authors showed that any vacuum state must vanish within finite time for the free boundary problem of the one-dimensional compressible Navier–Stokes equations with density-dependent viscosity with . This phenomenon implies the different behaviors for Navier–Stokes equations with different types of viscous effects, namely, degenerate or not.

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