Polymer-dispersed liquid crystals (PDLCs), consisting of a dispersion of LC-rich domains
in a polymer matrix, are used in different types of electrooptical devices. Their efficiency can in principle
be increased if the LC domains exhibit a uniform characteristic size in the range of the wavelength of
visible light. In an attempt to generate this type of morphology, a model PDLC system based on a 50 wt
% solution of N-4-ethoxybenzylidene-4‘-n-butylaniline (EBBA) in an epoxy monomer (diglycidyl ether of
bisphenol A, DGEBA) was analyzed. The polymerization-induced phase separation was performed at 80
°C, using a tertiary amine as initiator (benzyldimethylamine, BDMA). By selecting an initial concentration
located close to the critical composition to promote spinodal demixing, co-continuous morphologies were
obtained, which were rapidly fixed by gelation. The conversion of epoxy groups (p) was followed by near-infrared spectroscopy (NIR). At p = 0.28, phase separation took place as revealed by transmission optical
microscopy (TOM) and by the acceleration observed in the isothermal cure rate. Gelation took place at p
= 0.35, soon after the cloud point. Although the primary structure was arrested by gelation, the LC-rich
phase was continuously enriched in pure EBBA, as revealed by the increase in T
NI with conversion
monitored by differential scanning calorimetry (DSC). Co-continuous structures remained unmodified
after the storage of PDLCs for several months. The nematic range of the LC-rich phase at p = 1 was
comprised between 34 °C (melting point) and T
NI = 68 °C. A 57% of the initial LC was present in nematic
domains at 40 °C, as determined by the variation of the FTIR absorbance of a characteristic LC peak
between isotropic and nematic states. Therefore, a possible route to obtain PDLCs with a uniform
characteristic size of LC domains is to start with a composition close to the critical one and select conditions
to produce liquid−liquid demixing soon before gelation.