In this master thesis, we consider the solutions of Navier-Stokes equations on thin 3D domains of the formΩε=Ω×(0,εg(x1,x2)) = (0,l1)×(0, l2)×(0,εg(x1,x2)), where the top boundary is non-flat. We consider the following boundary conditions:" periodic boundary conditions on the lateral boundary and general Navier-friction boundary conditions on the top and the bottom boundary". Under the assumption that‖u0‖H1≤Cε-1/2,‖Mεu0‖L2≤C andsimilar assumptions on the forcing term, we show global existence of strongsolutions, here Mεu0=(Mu01,Mu02,0),Mu0i=1/εg∫0εgu0i(x1,x2,x3)dx3,i=1,2.Under the assumption that f is translation compact in L∞(0,∞;L(Ωε)3),byusing the method in [24], we show the existence of (local) attractor of strong solutions for 3D Navier-Stokes equations.
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