In subcritical and critical scalings, Navier-Stokes solutions in randomly perforated domains converge to Euler or Euler-Brinkman equations under small local Reynolds number.
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Homogenization of the Navier-Stokes equations in a randomly perforated domain in the inviscid limit
In subcritical and critical scalings, Navier-Stokes solutions in randomly perforated domains converge to Euler or Euler-Brinkman equations under small local Reynolds number.