Abstract
We consider a non-Newtonian flow in a thin domain of thickness ε. The flow is described by the 3D incompressible Navier–Stokes (Stokes) system with a nonlinear viscosity, being a power of the shear rate (power law) of flow index p.The bottom of the domain is irregular by the presence of slight roughness of amplitude εδ and period εβ, satisfying the relation 1<β<δ. Assuming pure slip or partial slip with a friction coefficient ε−γ, with γ>0, on the rough boundary, we consider the limit when domain thickness tends to zero and we obtain different models depending on the magnitude δ with respect to 2p−1pβ−p−1p, and the magnitude γ with respect to 1p−1.
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