The phase separation between two immiscible liquids advected by a bidimensi
onal velocity field is investigated numerically by solving the correspondin
g Cahn-Hilliard equation. We study how the spinodal decomposition process d
epends on the presence-or absence-of Lagrangian chaos. A fully chaotic how,
in particular, limits the growth of domains, and for unequal volume fracti
ons of the liquids, a characteristic exponential distribution of droplet si
zes is obtained. The limiting domain size results from a balance between ch
aotic mixing and spinodal decomposition, measured in terms of Lyapunov expo
nent and diffusivity constant, respectively.