On the dynamical Rayleigh-Taylor instability of non-homogeneous fluid in annular region with Naiver-slip boundary
Liang Li, Quan Wang
TL;DR
The paper analyzes the dynamical Rayleigh–Taylor instability for a 2D, nonhomogeneous incompressible Navier–Stokes system in an annulus with mixed boundary conditions, using polar coordinates to exploit the geometry. It establishes local well-posedness via a semi-Galerkin approach and Stokes estimates, and then demonstrates linear RT instability by separating variables and a modified variational method. Building on this, it proves nonlinear instability in both Lipschitz and Hadamard senses through detailed energy estimates and a variational construction of the maximum growth rate, valid under reasonably broad density profiles. The results illuminate the transition from linear growth to nonlinear breakdown in annular geophysical/astrophysical flows and provide rigorous instability criteria valuable for understanding stratified viscous fluids with slip boundaries.
Abstract
This paper investigates the well-posedness and Rayleigh-Taylor (R-T) instability for a system of two-dimensional nonhomogeneous incompressible fluid, subject to the non-slip and Naiver-slip boundary conditions at the outer and inner boundaries, respectively, in an annular region. In order to effectively utilize the domain shape, we analyze this system in polar coordinates. First, for the well-posedness to this system, based on the spectral properties of Stokes operator, Sobolev embedding inequalities and Stokes' estimate in the context of the specified boundary conditions, etc, we obtain the local existence of weak and strong solutions using semi-Galerkin method and prior estimates. Second, for the density profile with the property that it is increasing along radial radius in certain region, we demonstrate that it is linear instability (R-T instability) through Fourier series and the settlement of a family of modified variational problems. Furthermore, based on the existence of the linear solutions exhibiting exponential growth over time, we confirm the nonlinear instability of this steady state in both Lipschitz and Hadamard senses by nonlinear energy estimates.
