Inversion of the cyclohexane ring system in the solid state has been directly observed in a ' 9~ nmr study of solid fluorocyclohexane. The barrier to ring inversion in the orientationally disordered solid phase, AG+,,, = 44.1 k 0.9 kJ molpl at 263 K is found to be only slightly larger than the value previously reported for a CFC13 solution of fluorocyclohexane. The population of the equatorial conformation is slightly favored over the axial conformation with K = P,/Pa = 1.56 at 281 K; similar values have been obtained in CFCI3 and in the gas phase. RODERICK E. WASYLISHEN. Can. J. Chem. 64, 2094Chem. 64, (1986.Une Ctude par rmn du 19F du fluorocyclohexane B l'ttat solide a permis d'observer directement l'inversion du noyau cyclohexane ii 1'Ctat solide. On a trouvC que, a 263 K, la barrikre a I'inversion de cycle, dans le phase solide dCsordonnCe du point de vue de I'orientation, AG*,,, = 44,l L 0,9 k.J mol-', n'est que 1Cgerement supCrieure B la valeur rapportee antkrieurement pour une solution de fluorocyclohexane dans le CFC13. La population de la conformation Cquatoriale est lCgerement favorisCe par rapport a la conformation axiale et K = P,/Pa = 1,56, ii 281 K; des valeurs semblables ont Ct C obtenues pour des solutions dans le CFC13 ainsi qu'en phase gazeuse.[Traduit par la revue]In the gas phase (1, 2) and in solution (3-8) the cyclohexane ring of monosubstituted cyclohexanes is known to undergo rapid ring inversion (I). The transition state for this process is thought to involve a half-chair structure with boat and twist-boat forms existing as intermediates along the reaction path ( Fig. 1) (3,8-12). Typical barriers for ring inversion are 40-45 kJ mol-' while the energy differences between the equatorial and axial conformers are generally 0-4 kJ mol-' (3,7,8,13). Although some infrared and Raman evidence exists for ring inversion in solid cyclohexane (1 l), fluorocyclohexane, and chlorocyclohexane (14, 15), the rates of inversion have not been determined. Here we present preliminary results of a nmr study of solid fluorocyclohexane, which clearly demonstrate that the inversion process takes place in the solid state at rates comparable to those reported in CFC13 solutions (3).Representative variable temperature 19F nmr spectra of solid fluorocyclohexane are shown in Fig. 2. The spectra were obtained on a commercial sample (Cationics, Inc.) at 339.6736 MHz with 'H decoupling ( y B z = 2 kHz) using a Nicolet 360 nrnr spectrometer. The sample (mp = 285 K) was degrlssed and sealed under vacuum at 77 K in a 5-mm nmr tube. The relatively narrow nmr lines observed for solid fluorocyclohexane imply that it exists as an orientationally disordered solid between the mp and 183 ir 3 K. Below 183 +-3 K we were unable to detect a 1 9~ resonance because of dipolar broadening. A similar orientationally disordered solid phase is known to exist for cyclohexane between the mp (279.8 K) and 186.0 (16).The spectra in Fig. 2