The excess heat capacity, c:, has been measured through the concentration range at 25OC for cyclohexane + where R = methyl (Me), ethyl (Etj, propyl (Pr), and butyl (Bu). C: is negative and concave upward for the last three oxysilanes. For R = Me CE has a region of zero curvature, which, on reducing T to 2'C, becomes concave downward, i.e., its concentration dependence becomes W-shaped. C; has also been obtained at 15°C for Si(OMe)4 mixed with the following hydrocarbons of increasing molecular size: cyclooctane, cis-decalin, dicyclohexyl, n-hexadecane, 2,2,4,4,6,8,8-heptamethylnonane, 2,6,10,14-tetramethylpentadecane, and 2,6,10,15,19,23-heptamethyltetracosane (at 25OC). All CE values for these systems present a W-shape, which, with increasing hydrocarbon size becomes increasingly pronounced and moves to lower hydrocarbon concentration. C: behaviour correlates with degrees of non-randomness in the systems as quantified by the concentration-concentration correlation function S,, which is predicted using the Flory-Huggins theory with a group-interaction model and assuming interaction between molecular surfaces. Differences between C: for n-CI6 and highly branched C16 isomer, 2,2,4,4,6,8,8-heptamethylnonane, are attributed to liquid state orientational order and higher molecular surface/volume ratio for the normal isomer.Key words: excess heat capacity, W-shape, non-randomness, hydrocarbons, tetraalkylsiloxanes.LINA [Traduit par la revue]