The reaction of fluorine with CCl₃F has been studied over the temperature range 491–586 K. The mechanism is identical to that found in Pyrex vessels except that the reaction is now a homogeneous gas phase one. The rate equation has the form: –d[CCl₃F]/dt=k[F₂]^½[CCl₃F]. The rate constants fitted the Arrhenius equation: log k(1.^½ mol^–½ s^–1)=(11.95 ± 0.07)–(31490 ± 90)/2.303 RT where k=k₂(K_c)^½, k₂ is the rate constant for the reaction F + CCl₃F → ClF + CCl₂F and k_c is the equilibrium constant for the homogeneous gas phase dissociation of fluorine. This leads to D^°₀(CCl₂F—Cl)= 72 ± 2 kcal mol^–1 and ΔH^°_f0(CCl₂F)=–24 ± 4 kcal mol^–1. The temperature dependence of the ignition limits has been investigated, and treated by thermal explosion theory. The ignitions are shown to be the result of radical branching reactions brought about by the collisional deactivation of vibrationally excited CCl₂F₂ molecules. Induction periods were also observed and studied.