Abstract
The thermal decomposition of CF3H has been studied in a single‐pulse shock tube between 1200° and 1600°K using dilute CF3H–Ar mixtures at total pressures of about 18.7 and 0.90 atm. The results, together with earlier work at about 4 atm indicate that the observed rate constants for the rate of disappearance of CF3H are those of a second‐order energy‐transfer process, where collisional activation is rate determining. Kassel's model of unimolecular reaction‐rate theory is used to show that the observed pressure dependence of the rate constants is not unreasonable. From the classical Kassel theory for such processes it is calculated that the mean lifetime of a critically energized CF3H* at 1400°K is 1.2×10−11 sec with five effective oscillators.

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