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The aim of this article is to justify mathematically, in the two-dimensional periodic setting, a generalization of a two-phase model with pressure dependent viscosity first proposed by A. Lefebvre-Lepot and B. Maury to describe a system in one dimension of aligned spheres interacting through lubrication forces. This model involves an adhesion potential, apparent only on the congested domain, which keeps track of history of the flow. The solutions are constructed (through a singular limit) from a compressible Navier-Stokes system with viscosity and pressure both singular close to a maximal volume fraction. Interestingly, this study can be seen as the first mathematical connection between models of granular flows and models of suspensions. As a by-product of this result, we also obtain global existence of weak solutions for a system of incompressible Navier-Stokes equations with pressure dependent viscosity, the adhesion potential playing a crucial role in this result.

Pressure-Dependent Viscosity Model for Granular Media Obtained from Compressible Navier–Stokes Equations