Abstract

We consider the compressible Navier-Stokes system describing the motion of a viscous fluid confined to a straight layer Ωδ=(0,δ)×R2Ω_δ=(0,δ)\times\mathbb{R}^2. We show that the weak solutions in the 3D domain converge strongly to the solution of the 2D incompressible Navier-Stokes equations (Euler equations) when the Mach number εε tends to zero as well as δ→0δ\rightarrow 0 (and the viscosity goes to zero).

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