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Benzene dimer has long been an archetype for π-stacking. According to the Hunter-Sanders model, quadrupolar electrostatics favors an edge-to-face CH⋯π geometry but competes with London dispersion that favors cofacial π-stacking, with a compromise "slip-stacked" structure emerging as the minimum-energy geometry. This model is based on classical electrostatics, however, and neglects charge penetration. A fully quantum-mechanical analysis, presented here, demonstrates that electrostatics actually exerts very little influence on the conformational landscape of (C 6 H 6 ) 2 . Electrostatics also cannot explain the slip-stacked arrangement of C 6 H 6 ⋯C 6 F 6 , where the sign of the quadrupolar interaction is reversed. Instead, the slip-stacked geometry emerges in both systems due to competition between dispersion and Pauli repulsion, with electrostatics as an ambivalent spectator. This revised interpretation helps to rationalize the persistence of offset π-stacking in larger polycyclic aromatic hydrocarbons and across the highly varied electrostatic environments that characterize π-π interactions in proteins.

Electrostatics does not dictate the slip-stacked arrangement of aromatic π–π interactions