Abstract:
The Enskog–Vlasov equation is a phenomenological kinetic equation that extends the
Enskog equation for the dense (non-ideal) hard-sphere fluid by adding an attractive soft
potential tail to the purely repulsive hard-sphere contribution. Simplifying assumptions
about pair correlations lead to a Vlasov-like self-consistent force field that adds to the
Enskog non-local hard-sphere collision integral. Within the limitations imposed by the
underlying assumptions, the extension gives the Enskog–Vlasov equation the ability to
give a unified description of ideal and non-ideal fluid flows as well as of those fluid
states in which liquid and vapour regions coexist, being separated by a resolved interface.
Furthermore, the Enskog–Vlasov fluid can be arbitrarily far from equilibrium. Thus the
Enskog–Vlasov model equation provides an excellent, although approximate, tool for
modelling processes with liquid–vapour interfaces and adjacent Knudsen layers, and
allows us to look at slip, jump and evaporation coefficients from a different perspective.
Here, a set of 26 moment equations is derived from the Enskog–Vlasov equation by means
of the Grad moment method. The equations provide a meaningful approximation to the
underlying kinetic equation, and include the description of Knudsen layers. This work
focuses on the – rather involved – derivation of the moment equations, with only a few
applications shown.