Depending upon the ranges of attractive and repulsive interactions between
molecules, the transition from the liquid expanded to the condensed phase c
an be either horizontal or inclined. When the attractive interaction has a
much longer range than the repulsive one, thermodynamics favors the aggrega
tion of the molecules of the condensed phase in a single large aggregate, a
nd a first order, horizontal transition will occur. When the repulsive inte
raction has the much longer range, the free energy of the system becomes sm
aller when the new phase is dispersed as islands in the old one, instead of
forming a separate bulk phase, and a nonconventional first order, inclined
transition will take place. It is likely that the phospholipid monolayers
belong to the latter kind, while the fatty acid monolayers to the former, w
hen they are little dissociated (sufficiently low pH values), and to the la
tter, when they are dissociated (sufficiently high pH values). A thermodyna
mic approach is employed to explain the nonhorizontal transition from the l
iquid expanded to the condensed phase. A modified Clausius-Clapeyron equati
on is derived for this nonconventional first order transition. (C) 2001 Els
evier Science B.V. All rights reserved.