the wave vector q, one finds with short-chain amphiphiles Z(q) to drop monotonically. Upon increasing ( i , j ) , one observes a gradual evolution of a correlation peak (Fig. 19 in [I]), followed by a q -4 decay for large q (Porod's law). As Teubner and Strey [I21 have shown, the curves can be fitted rather well bywith a < 0, and b > 0. With increasing (i, j ) , the position of the peak moves gradually towards lower q, with the q -4 decay becoming increasingly wider. The evolution of the peak indicates a gradual evolution of a characteristic periodicity d in the mixture that increases with increasing ( i , j ) , while the fact that Porod's is increasingly better obeyed indicates that the scattering length density gradient at the interfaces becomes increasingly steeper. If d is interpreted as mean distance between the centers of the dispersed domains, a simple calculation [I31 shows that the position of the peak is solely determined by the mass balance, irrespective of the model used for describing the mixtures.I am indebted to all of my coworkers for their assistance with the experiments, and their contributions to the discussions.The hard sphere dipole fluid shows an instability towards formation of oriented clusters in the vapour before condensation. The coexistence interface profile is derived from a WDA approximation of the direct correlation function. Integration of the equation for V p yields also the orientation of the dipoles near the interface.