  The microscopic mechanisms for universality of Casimir forces between
macroscopic conductors are displayed in a model of classical charged fluids.
The model consists of two slabs in empty space at distance $d$ containing
classical charged particles in thermal equilibrium (plasma, electrolyte). A
direct computation of the average force per unit surface yields, at large
distance, the usual form of the Casimir force in the classical limit (up to a
factor 2 due to the fact that the model does not incorporate the magnetic part
of the force). Universality originates from perfect screening sum rules obeyed
by the microscopic charge correlations in conductors. If one of the slabs is
replaced by a macroscopic dielectric medium, the result of Lifshitz theory for
the force is retrieved. The techniques used are Mayer expansions and integral
equations for charged fluids.
