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Global weak solutions and incompressible limit to the isentropic compressible Navier-Stokes equations in the half-plane with ripped density and large initial data

Shuai Wang, Guochun Wu, Xin Zhong

TL;DR

The paper addresses global existence of weak solutions and the incompressible limit for the isentropic compressible Navier–Stokes equations in a half-plane with ripped density and slip boundary. The authors develop a two-tier approach that yields uniform a priori control, notably via a Desjardins-type logarithmic interpolation inequality and the effective viscous flux, to handle large bulk viscosity and vacuum. They prove the existence of a global weak solution with controlled density for large initial energy when $\lambda$ is sufficiently large, and show that, as $\lambda\to\infty$, a subsequence converges to a weak solution of the inhomogeneous incompressible Navier–Stokes equations with $\operatorname{div}\mathbf{v}=0$ on compact sets. This work extends prior incompressible-limit results to a boundary-rich half-space, accommodating vacuum and nonzero initial momentum, and clarifies the boundary’s role in the limit behavior.

Abstract

We prove the global existence of weak solutions to the isentropic compressible Navier-Stokes equations with ripped density in the half-plane under a slip boundary condition provided the bulk viscosity coefficient is properly large. Moreover, we show that such solutions converge globally in time to a weak solution of the inhomogeneous incompressible Navier-Stokes equations as the bulk viscosity coefficient tends to infinity. In particular, the large initial data and an initial patch of density as well as a vacuum are allowed. Our method relies on a Desjardins-type logarithmic interpolation inequality and some new techniques based on the effective viscous flux.

Global weak solutions and incompressible limit to the isentropic compressible Navier-Stokes equations in the half-plane with ripped density and large initial data

TL;DR

The paper addresses global existence of weak solutions and the incompressible limit for the isentropic compressible Navier–Stokes equations in a half-plane with ripped density and slip boundary. The authors develop a two-tier approach that yields uniform a priori control, notably via a Desjardins-type logarithmic interpolation inequality and the effective viscous flux, to handle large bulk viscosity and vacuum. They prove the existence of a global weak solution with controlled density for large initial energy when is sufficiently large, and show that, as , a subsequence converges to a weak solution of the inhomogeneous incompressible Navier–Stokes equations with on compact sets. This work extends prior incompressible-limit results to a boundary-rich half-space, accommodating vacuum and nonzero initial momentum, and clarifies the boundary’s role in the limit behavior.

Abstract

We prove the global existence of weak solutions to the isentropic compressible Navier-Stokes equations with ripped density in the half-plane under a slip boundary condition provided the bulk viscosity coefficient is properly large. Moreover, we show that such solutions converge globally in time to a weak solution of the inhomogeneous incompressible Navier-Stokes equations as the bulk viscosity coefficient tends to infinity. In particular, the large initial data and an initial patch of density as well as a vacuum are allowed. Our method relies on a Desjardins-type logarithmic interpolation inequality and some new techniques based on the effective viscous flux.

Paper Structure

This paper contains 10 sections, 14 theorems, 160 equations.

Key Result

Theorem 1.1

Let z1.8 and z1.9 be satisfied, there exists a positive number $D$ depending only on $\tilde{\rho}$, $\hat{\rho}$, $a$, $\gamma$, and $\mu$ such that if then the problem a1--a4 admits a global weak solution $(\rho,\mathbf{u})$ in the sense of Definition d1.1 satisfying where $\sigma\triangleq\min\{1,t\}$.

Theorems & Definitions (30)

  • Definition 1.1
  • Theorem 1.1
  • Theorem 1.2
  • Definition 1.2
  • Remark 1.1
  • Remark 1.2
  • Remark 1.3
  • Remark 1.4
  • Lemma 2.1
  • Lemma 2.2
  • ...and 20 more