We present a theoretical analysis of a model nucleation process where
an oil phase separates out from a droplet microemulsion phase. We cons
ider a homogeneous nucleation where aggregate growth occurs through ad
dition of monomers. The nucleus is formed by the growth of an already
existing microemulsion droplet. On the basis of previous equilibrium s
tudies of the microemulsions of the same system we can be confident ab
out the accuracy of the description of free energy changes during nucl
eation. Using the constraints of constant hydrocarbon volume and aggre
gate area, the change in curvature free energy is determined as an oil
drop is nucleated rather than the change in surface free energy, as i
n a conventional nucleation theory. We obtain a simple analytical expr
ession for the barrier which has the feature that it only exists in a
finite parameter range. In the particular system that we have studied
experimentally a two-phase system of microemulsion plus excess oil is
reached through a temperature quench and a nucleation barrier is found
for moderately deep quenches only. Having established an expression f
or the nucleation barrier, we analyze the kinetics and derive a diffus
ion equation in aggregate space, which considerably facilitates the ca
lculation of the steady state rate for the formation of nuclei. Experi
ments confirm the existence of a nucleation barrier in the predicted r
ange. They also show the concentration independence of the barrier and
that experiments with different initial radii can be put on a common
scale, as predicted. It is concluded that the system is very promising
for fundamental studies of the dynamics of nucleation processes in li
quids.