ABSTRACT:The misciblity of ternary blends consisting of amorphous nylon (Am-Nylon)lpoly(methyl methacrylate) (PMMA)Ipoly(4-vinylphenol) (PVPh) at 190°C was investigated by differential scanning calorimetry (DSC),thermo-photometry, Fourier transform infrared spectroscopy (FT-IR), and scanning electron microscopy (SEM). In the ternary blends, more than 70-90wt% PVPh was required to cause miscibility between Am-Nylon and PMMA, and the experimental ternary diagram indicating symmetrically miscible regions was obtained. FT-IR results showed this miscibility was attributed to intermolecular hydrogen bonding interactions. Using stoichiometric equations, the equilibrium constant (Kc = 3.2) describing hydrogen bonding between the OH group of PVPh and amide group of Am-Nylon was determined from quantitative FT-IR analysis. The miscible region was affected by individual equilibrium constants (K;), since individual binary interaction parameters (Xii) were significantly larger than the critical value of Xii· The miscibility of Am-NyloniPMMA blends was enhanced by adding 20wt% PVPh to binary immiscible polymer. Recently, due to the industrial importance of multicomponent blends, the miscibility and morphology of ternary blends have been investigated. 1 -7 By ternary blends one could obtain more polymer composites than binary blends, having high ability and faculty. However, it is clear that the complexity of calculating phase diagrams, problems of experimental accuracy and interpretation of results of ternary blends increase dramatically over that of analogous binary blends.The phase behavior of ternary polymer blends involving strong specific interactions (hydrogen bonding), has only been studied by Coleman, Pomposo, and others. 8 -11 A binary association model which was suggested by Coleman et al., and has been extended to ternary hydrogen bonding polymer mixtures. This model was based on the suggestion to separate favorite 'chemical' specific interactions from unfavorite 'physical' ones. 12 -1 7 The free energy of mixing !lG m of ternary systems can be expressed in eq 1 by adding free energy (!lG:,H) of mixing based on the Flory-Huggins theory (2) where