“…To incorporate the influence of intermolecular interactions to the ideal situation (eqs 14 and 15), from a theoretical point of view, is usually assumed the so-called “mean-field approximation”, which considers that all adsorbates on the surface lattice are randomly mixed and uncorrelated. 50 As a result, the average interaction energy that an adsorbate feels from the others is proportional to the coverage f . If we restrict to the nearest-neighbor interactions, an additional energy term should be added to the electrochemical potential, thus giving rise to the Frumkin isotherm, which for two adsorbates O and R and an electroinactive coadsorbate P takes the following expression 51
with a OO , a RR , a OR , a OP , and a RP being the interaction coefficients for couples O–O, R–R, O–R/R–O, OP, and RP, respectively (with a ij being positive for attractions and negative for repulsions 30 ).…”