“…The renormalized fluid is one with the effective dipole moment (rather than the value in vacuo) and with no polarizability, and the problem is thus rephrased in terms of two‐body and three‐body correlations. The theory was extended to mixtures and comprehensively described by Venkatasubramanian et al,20 Joslin et al,21 and Gray et al22 If we restrict our considerations to bulk properties (excluding the dielectric behavior of a fluid), the RPT, despite its elegance, was next applied only a decade later, when Kriebel and Winkelmann23–25 developed an equation of state for polarizable spherical and polarizable two‐center Lennard‐Jones molecules with embedded dipole moment. They used a simplified implementation of RPT and compared their model to their own molecular simulation data.…”