The pair correlation function g((2))(r) in a classical many-body system dep
ends in a nontrivial way both on the number density rho and on the pair int
eractions v(r), and a long-standing goal of statistical mechanics has been
to predict these effects quantitatively. The present investigation focuses
on a restricted circumstance whereby simultaneous isothermal changes in rho
and v(r) have exactly canceling effects on g(2). By appealing to the isoth
ermal compressibility relation, we establish that an upper limit for densit
y increase exists for this "iso-g((2))" process, and at this limit in three
dimensions the correspondingly modified pair interaction develops a long-r
anged Coulombic character. Using both the standard hypernetted chain and Pe
rcus-Yevick approximations, we have examined the iso-g((2)) process for rig
id rods in one dimension that starts at zero density, and maintains the sim
ple step-function pair correlation during density increase, a process that
necessarily terminates at a covering fraction of one-half. These results ha
ve been checked with detailed Monte Carlo simulations. We have also estimat
ed the effective pair potentials that are required for the corresponding ri
gid-sphere model in three dimensions, for which the simple step-function pa
ir correlation can be maintained up to a covering fraction of one-eighth.