INTRODUCTIONlated in the same manner by substituting the number of reactive carbon atoms to the functionality [i.e., for each C|C present this gives two reactive carbons, and Molecular mechanics in the broader sense of the term thus a Å 1/( f 0 1 ), where f is 2 rather than 1 as it is a computational technique that is, among its other would be in polycondensates 8 ]. applications, particularly suited for determining at the Although interesting conclusions about the covalent molecular level the interactions at the interface of monetworking of polymers, both polycondensates and othlecularly well-defined polymers. It has already been ers, 9 have already been obtained, some equally interused in the wood field, for instance, to calculate the esting considerations on the interfacial adhesion berelative energies of interaction between synthetic polytween an adhesive and a lignocellulosic substrate, and condensation oligomers used as adhesives and their celby inference on the interfacial adhesion between any lulosic substrate with excellent correspondence betwo materials, can also be derived. This article, then, tween calculated and applied results and some interestaddresses this aspect of the above formula's applicaing applied consequences, 1-6 as well as to address other tion. interfacial energy problems. Recently, an equation, as well as its simpler regressions, correlating the relative deflection obtained by thermomechanical analysis with the sum of the interfa-EXPERIMENTAL cial energy of interaction of a synthetic polymer with wood plus the internal cohesive strength of the hardMaterials ened synthetic polymer has been obtained, [8][9][10] namely Three photopolymerizable primer monomers, namely E Å 0km/(af ) the linear hexanediol diacrylate (HDDA ), the branched trimethylol propane triacrylate (TMPTA) and the linwhere k is a constant dependent upon the testing condiear tripropyleneglycol diacrylate (TPGDA), supplied tions used, m is the average number of degrees of freeby CIBA-GEIGY, Basel, Switzerland, and a model of a dom between crosslinking nodes of a hardened network, linear unsaturated polyester -alkyd varnish repeating E is the sum of the energy of interaction at the interface unit, were used for the study. The following polycondenof the synthetic polymer and the substrate and of the sation resins were used: (1 ) An industrial pure resorinternal cohesive energy of the synthetic polymer (the cinol-formaldehyde (RF) cold set resin having a solids internal energy of the substrate is not considered becontent of 53%, a pH of 8.3, and a manufacturing molar cause the deflection measured is relative to the subratio R : F of 1 : 1.5, to which was added one further strate alone ), and a is Flory's coefficient of branching molar proportion of paraformaldehyde as hardener to for polycondensates. The above equation has been yield a final molar ratio R : F of 1 : 2.5, supplied by shown to work also for radical hardening polymers, Bakelite AG (Duisburg-Meiderich), Germany, and spewith the proviso that the coefficient a is n...