Vanishing shear viscosity and boundary layers for plane magnetohydrodynamics flows

In this paper, we consider an initial-boundary problem for plane magnetohydrodynamics flows under the general condition on the heat conductivity $κ$ that may depend on both the density $ρ$ and the temperature $θ$ and satisfies $κ(ρ,θ)\geqκ_1(1+θ^{q}) \quad \hbox{\rm with constants}~ κ_1>0 ~\hbox{\rm and}~ q>0.$ We prove the global existence of strong solutions for large initial data and justify the passage to the limit as the shear viscosity $μ$ goes to zero. Furthermore, the value $μ^α$ with any $0<α<1/2$ is established for the boundary layer thickness.

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