The correspondence between the equilibrium phase behavior of oil-water
-surfactant mixtures and the macroemulsion type and stability is exami
ned. Both the phase behavior and emulsion stability are argued to be d
ependent on the bending elasticity of the surfactant monolayer at the
oil-water interface. At positive spontaneous curvatures, O/W emulsions
are stable; at negative spontaneous curvatures W/O emulsions are stab
le, whereas, in the balanced state of the surfactant film, an emulsion
break usually occurs for a wide variety of systems. To explain the ef
fect of the monolayer bending properties on the macroemulsion stabilit
y, the thermally activated rupture of emulsion films is theoretically
studied. We consider emulsion films covered by saturated surfactant mo
nolayers, with strong lateral interactions among the adsorbed surfacta
nt molecules. The monolayer at the edge of a nucleation hole in the em
ulsion film is strongly curved; the bending energy penalty involved le
ads to a strong dependence of the coalescence barrier on the sign and
the absolute value of the monolayer spontaneous curvature. By contrast
with earlier hole nucleation theories, the emulsion film thickness is
allowed to vary, in order to minimize the free energy of the nucleati
on hole. At large positive spontaneous curvatures, Ho, the oil-water-o
il (O/W/O) films are stable, with a coalescence barrier, in a first ap
proximation, proportional to the bending modulus kappa. On the other h
and, W/O/W films break without a barrier. Conversely, for large negati
ve values of Ho, W/O/W films are stable, while O/W/O films break witho
ut a barrier. In the vicinity of the balanced state, a very steep chan
ge in film stability with Ho is predicted. The model reproduces the ma
croemulsion stability sequence: O/W emulsion-emulsion breakage-W/O emu
lsion, observed in polyethoxylated nonionic surfactant-oil-water mixtu
res with increasing temperature. The macroemulsion break is predicted
to occur at the balanced (PIT) point, as has been observed experimenta
lly by Shinoda et al. The hole nucleation in multilamellar-stabilized
films is shown to be drastically suppressed, in agreement with the exp
erimental findings of Friberg et al. For rigid surfactant monolayers (
kappa similar to 100 kT) and multilamellar-stabilized systems, a regio
n of stable multiple emulsions is predicted, while it is prohibited fo
r flexible (kappa similar to 1 kT) monolayers. Possible extensions of
the model to other systems are discussed.