“…According to the Demchak-Fort model [20], µ ⊥ is composed of three independent contributions arising from (i) orientation of water dipoles in the vicinity of the headgroups, (ii) the headgroup dipoles, and (iii) the hydrophobic part dipoles. Moreover, in our calculations we assumed, as it is made customary [19,21], that ε r = 1, although it is known that dipoles in a monolayer may be embedded in media with distinct, nonunity dielectric constant values, which depends on whether these dipoles are at the monolayer-water or monolayer-air interface [22,23].…”