H. Kellay et al., PROPERTIES OF SURFACTANT MONOLAYERS IN RELATION TO MICROEMULSION PHASE-BEHAVIOR, Advances in colloid and interface science, 49, 1994, pp. 85-112
The relationship between the properties of surfactant monolayers at oi
l-water interfaces and the phase behaviour in bulk of mixtures of oil
+ water + surfactant is discussed. Such monolayer properties include t
he spontaneous curvature, c(o), the interfacial, tension, gamma, the e
lasticity K (or rigidity) associated with the mean curvature, and the
elasticity KBAR associated with the Gaussian curvature. The model syst
em chosen for investigation is the anionic surfactant AOT + aqueous Na
Cl + n-alkane at 20-degrees-C. In such systems, inversion of microemul
sion type from oil-in-water (o/w) to water-in-oil (w/o) is possible wi
th increasing electrolyte concentration. The tension, gamma, passes th
rough an ultralow minimum value at conditions corresponding to the for
mation of three phases. Using small angle neutron scattering, we have
determined the structure of surfactant-rich third phases (c(o) approxi
mately 0) formed with the different alkanes. Lamellar phases consistin
g of surfactant monolayers separated alternately by oil and water appe
ar with short alkanes, whereas L3 and bicontinuous phases form in syst
ems containing longer alkanes. The bending elasticity K has been measu
red for planar monolayers at the oil-water interface by ellipsometry.
K is independent of salt concentration but depends markedly on alkane
chain length N, falling from approximately 1 k(B)T for N < 11 to appro
ximately 0.1 k(B)T for N = 14. This is discussed in terms of the diffe
ring extents of oil penetration into the surfactant chains. Higher rig
idities favouring lamellar phases and lower rigidities favouring bicon
tinuous microemulsions are in line with the theoretical predictions of
de Gennes and Taupin. Estimates of the constant KBAR have been obtain
ed in droplet microemulsions (w/o) from a knowledge of their size, K a
nd gamma. The sign of the constant is in agreement with the geometry o
f the phases formed in three phase systems. Finally, the ideas and con
cepts developed in the oil-water systems described above are used to e
xplain the wetting behaviour by alkanes of AOT monolayers at the air-w
ater surface.