This discussion addresses an important issue related to gases, which are known to be one of the fourth states of matter (gases, liquids, solids, and plasmas).
We learn from high school the ideal gas of equation of state, where particles are considered point particles, non-interacting, and massless (sometimes).
Even though using that simple model, many nontrivial questions that help to understand more complicated models can be answered for all Statistics, from the classical Gibbs and Maxwell Boltzmann distributions that obey Gaussian curves, where even degeneracy can be taken to be part of the exercise; to the more complicated Fermi-Dirac and Bose-Einstein statistics; where quantum effects are unavoidable, even if the gas is considered a free gas of electrons, or bosons non-interacting quasiparticles.
But what happens when the expansion terms are higher than for a simple gas and interactions are taken into account?
"What classical and/or effects survive from the ideal gas model and what has to be modified?" arises.
The question can be addressed for statistical equilibrium thermodynamics but also can be part of non-equilibrium statistical thermodynamics.
This science popularization thread will discuss some issues, as well as, some historical points in the development of this interesting subject, which belongs to exact and applied sciences as is the real gases issue.
Some new and old references cover some applied and theoretical aspects that will be addressed here. They are: