2017
DOI: 10.1016/j.jde.2016.11.021
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Stability of stationary solution for the compressible viscous magnetohydrodynamic equations with large potential force in bounded domain

Abstract: In this paper, we consider the 3-D compressible viscous magnetohydrodynamic (MHD) equations with some large potential force in bounded rigid vessel. We firstly construct the non-constant stationary solutions of the compressible viscous MHD equations under suitable constitutive assumptions. Next, a critical energy identity is established to achieve a universal stability criterion of the stationary solution. In this case, the stationary solution is exponential stable for any large external potential force. Final… Show more

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Cited by 8 publications
(2 citation statements)
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“…In this paper, we consider the following compressible magnetohydrodynamic equations in R3 (see other studies() for instance): ρt+divfalse(ρufalse)=0, ρut+divfalse(ρuufalse)+Pfalse(ρfalse)=false(×Hfalse)×H+μnormalΔu+false(μ+λfalse)divu+ρf, Ht×false(u×Hfalse)=×false(ν×Hfalse), divH=0, with x=false(x1,x2,x3false)R3, t ≥ 0. The unknown functions ρ , u = ( u 1 , u 2 , u 3 ), P , H = ( H 1 , H 2 , H 3 ), and f = ( f 1 , f 2 , f 3 ) represent the density, the velocity, the pressure, the magnetic field, and the (assigned) external force field, respectively.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…In this paper, we consider the following compressible magnetohydrodynamic equations in R3 (see other studies() for instance): ρt+divfalse(ρufalse)=0, ρut+divfalse(ρuufalse)+Pfalse(ρfalse)=false(×Hfalse)×H+μnormalΔu+false(μ+λfalse)divu+ρf, Ht×false(u×Hfalse)=×false(ν×Hfalse), divH=0, with x=false(x1,x2,x3false)R3, t ≥ 0. The unknown functions ρ , u = ( u 1 , u 2 , u 3 ), P , H = ( H 1 , H 2 , H 3 ), and f = ( f 1 , f 2 , f 3 ) represent the density, the velocity, the pressure, the magnetic field, and the (assigned) external force field, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Assume that the large potential force satisfy f = ( f 1 ( x ), f 2 ( x ), f 3 ( x )), Li and Yang studied the well‐posedness of the initial boundary value problem for the compressible viscous MHD equations provided that the initial data are close to the stationary solution. However, the condition that the initial density ρ 0 in Li and Yang has positive lower bound is quite essential, ie, no vacuum at any point.…”
Section: Introductionmentioning
confidence: 99%