HELMUT BEIERBECK and JOHN K. SAUNDERS. Can. J. Chem. 55, 771 (1977). The conformations of saturated hydrocarbon chains are analysed by a least-squares fit of calculated to observed time-averaged carbon-13 chen~ical shifts. The calculated resonances are the sums of products of conformer resonances and conformer probabilities. The conformer shieldings are derived with predictive parameters developed earlier for conformationally well defined systems. The conformer probabilities are taken to be products of rotamer probabilities. The rotamer probabilities are variables in the analysis. The carbon-13 resonances of saturated hydro-carbons is based on four separate reference carbon chains at ambient temperatures are the values, since a-carbon substituent effects are sums of the chemical shifts in all molecular nonadditive. The resonances of the primary, conformations, weighted by the probability of secondary, tertiary, and quaternary carbons in occurrence of each conformation. If the con-ethane, propane, isobutane, and neopentane, former resonances may be measured, or cal-respectively, served as starting estimates for culated to a good approximation, the conformer these references. Two substituent parameters, populations may be derived by fitting calculated HC and CC, account for the deshielding effect to observed time-averaged carbon-13 resonances. of P-carbons. A shift increment HC is associated Since conformational analysis is a prerequisite with every 1,3-diaxial hydrogen-hydrogen interfor the determination of the configurations of action introduced by a P-carbon. An increment mobile systems, the derivation of the conforma-CC is associated with everv carbon-carbon tional probabilities from time-averaged carbon-gauche interaction. Previously derived parameter 13 resonances also allows the determination of values (2, 3) served as starting estimates for HC configuration in asymmetric hydrocarbon chains. and CC. No y-carbon parameter is required.