Abstract
In this paper, we study a class of analytical solutions to the 3-D compressible Navier-Stokes equations with density-dependent viscosity coefficients, where the shear viscosity $h(\rho)=\mu\geq0$ , and the bulk viscosity $g(\rho)=\rho^{\beta}$ ( $\beta>0$ ). By constructing a class of radial symmetric and self-similar analytical solutions in $\mathbb {R}^{N}$ ( $N\geq2$ ) with both the continuous density condition and the stress free condition across the free boundaries separating the fluid from vacuum, we derive that the free boundary expands outward in the radial direction at an algebraic rate in time and we also have shown that such solutions exhibit interesting new information such as the formation of a vacuum at the center of the symmetry as time tends to infinity and explicit regularities, and we have large time decay estimates of the velocity field.
Highlights
The compressible Navier-Stokes equations with density-dependent viscosity coefficients can be written as ⎧⎨∂tρ + div(ρU) =, ⎩∂t(ρU) + div(ρU ⊗ U) – div(h(ρ)D(U)) – ∇(g(ρ) div U) + ∇P(ρ) =, ( . )where ρ(x, t), U(x, t), and P(ρ) = ργ (γ > ) stand for the fluid density, velocity, and pressure, respectively
The important progress on the global existence of strong or weak solutions in one spatial dimension or multi-dimension has been made by many authors; refer to [ – ]
For the periodic problem on the torus T and under assumptions that the initial density is uniform away from vacuum and β > where h(ρ) is a positive constant and g(ρ) = ρβ, Vaigant-Kazhikhov found the well-posedness of the classical solution to ( . ), and the global existence and large time behavior of weak solutions was studied by Perepelitsa in [ ]
Summary
The compressible Navier-Stokes equations with density-dependent viscosity coefficients can be written as Wang et al Boundary Value Problems (2015) 2015:94 tence and behaviors of solutions to The studies in Hoff and Serre [ ], Xin [ ], and Liu et al [ ] prove that the compressible Navier-Stokes equations with constant viscosity coefficients behave singularly in the presence of a vacuum.
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