Abstract
In this paper, we validate the boundary layer theory for 2D steady viscous incompressible magnetohydrodynamics (MHD) equations in a domain {(X,Y)∈[0,L]×R+} under the assumption of a moving boundary at {Y=0}. The validity of boundary layer expansions and convergence rates are established in Sobolev sense. We extend the results for the case with the shear outer ideal MHD flows [3] to the case of the nonshear flows.
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