Abstract

We present the convergence of (ρnγ) to ργ in compressible isentropic Navier–Stokes equations (Lions, 1996 [6]) in a domain which changes with time. The essential point is to show the convergence a.e. of the density. Following the proof of P.L. Lions, we prove that r=ρlogρ¯−ρlogρ (resp. r=ρ−(ρθ¯)1/θ) is equal to zero. In the case of a moving bondary problem, the main difficulty comes from the non homogeneous boundary condition on u⋅n.

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