According to percolation theory / I / , the study of the electron motion between localized states, which are randomly distributed in energy and position, in a disordered system, is equivalent to the study of the possibility of the passage of electric current through a network of impedances, Z.., which connect different lattice sites, i and j . Impedances of magnitude Zij *Zc, where Zc is the critical impedance, interconnecting small clusters of low impedances, form ak conductive cluster through the material.The inverse of the magnitude of impedances Z.. @ Zc, characterizes the A critical path of bonds can be constructed if the average number of bonds per site exceeds a certain critical value / 2 , 31. In this construction it is assumed that all sites are equivalent. When the site energies are not the same, the energy of a site affects the incoming as well as the outgoing 2'6, and this correlates neighboring Z's .Triberis and Friedman / 4 , 5 I , presented, using percolation theory, two methods for the calculation of the conductivity of the small polaron hopping regime in a disordered system. In the first they ignored correlations, while in the second they took correlations into account. Comparing these methods very useful conclusions were obtained and their results show how drastically correlations affect the temperature dependence of the conductivity. Using the generalized molecular crystal modes (GMCM) 14, 6, 71, they applied percolation theory to the high-temperature multiphonon-assisted small-polaron hopping regime in a disordered system (TF model I ) . They found / 4 / that the conductivity of the material varied as lncw [-(TAIT) ( 1) where T A = 8.5 N~12a3/2(kgNo) Here N is the concentration of sites, No the density of states, a-1 the spatial S ) Panepistimioupolis, G-15771 Zografou, Athens, Greece. ) Present address :