“…There is no adequate and simple microscopic theory of liquids to easily describe the conformational and external contributions. 6,7 It was, however, empirically found that C p L is often a linear function of temperature. Using the addition scheme developed for ATHAS, the total heat capacity of liquid state (C p L ) in J K Ϫ1 mol Ϫ1 can be obtained from contributions of the structural units as: 11,12 (4) where N are the numbers of the respective groups in the repeating unit of the PEIM-ns and the functions in the parentheses represent the contributions of the structural units to the total heat capacity at temperature T. The heat capacities of the liquid state of each structural unit was established from the prior data on liquid polyethylene, poly(ethylene terephthalate), and poly(oxyethyleneoxy-1,3-phenylene-4,4Ј-oxydiphthalimide-1,4-phenylene) contained in the ATHAS data bank.…”