Fluid flow that occurs when the Knudsen number, Kn, is in the range 0.01<Kn<0.1. As a result of rarefaction effects in the
Knudsen layer the no slip boundary condition fails. The flow outside the Knudsen layer can be represented by the continuum Navier–Stokes equations provided that an appropriate slip boundary condition is used for the fluid flow and the correct temperature jump boundary condition is applied at the interface.
Fluid flow that occurs when the Knudsen number, Kn, is in the range 0.1<Kn<10. In this regime, the flow is so rarefied that continuum equations break down completely. However, collisions between the molecules are still important so free molecular flow is not applicable.