. Can. J. Chem. 70, 849 (1992).A ' H and NMR study of the solid methylammonium hexahalotellurates, (MA),TeX6 (MA = C H 3~D 3 + or CD3NH3+, X = C1, Br, and I), has been undertaken to characterize the dynamics of the methylammonium (MA) ion as a function of temperature. At room temperature, the MA ion in the hexachlorotellurate (solid 11) is confined to C3 jumps about the C-N axis while a small angle libration of the C-N axis is occurring. In the room temperature phase, solid I, of (MA),TeBr6 and (MA),Te16 the MA ions are performing overall reorientations on the ps time scale, averaging the 'H nuclear quadrupolar interactions to zero. Variable temperature 'H NMR spin-lattice relaxation times, T I , indicate an activation energy, EA, for u i~~t r~p i c n reorientations of the CH3ND3+ ion of 5.2 ? 0.5 and 2.6 ? 0.3 kJ mol-I for X = Br and I, respectively. Deuterium TI values for C-deuterated MA ion in the hexaiodotellurate indicate an E, for whole-ion reorientation of 3.1 + 0.3 kJ mol-'. At any given temperature, the correlation time, T,, derived from the TI results was found to be the same for the two deuterium-labelled hexaiodotellurates. The similarity of both the E, and the T, values implies correlated motion of the methyl and ammonium groups. The ' 4~ TI results for solid I of (MA),Te16 indicate that C-N axis motions, with an EA = 5.6 + 0.6 kJ mol-', are more hindered than N-D or C-D bond dynamics. The ' H NMR spectra for (MA),Te16 (solid 11) and (MA),TeBr6 (solids 11, 111, and IV) are characterized by a Pake doublet line shape. The measured peak-to-peak splittings are less than what is predicted by C3 motion about the molecular symmetry axis. It is possible to model these line shapes by postulating that C3 rotations of the methyl and ammonium groups occur as the C-N axis librates in an effective cone about the position of the static molecular axis. For (CH3ND3),TeBr6 and (CD3NH3),TeBr6 the peak-to-peak splittings in the 'H NMR spectra were measured as a function of temperature in solid phases 11, 111, and IV and were found to be similar. Finally, the 'H NMR line shape relaxation for (MA)'TeBr6 (solid 111) displays an orientation dependence indicating that rotations about the C-N axis are discrete rather than diffusive in nature. For solid phase I1 of (MA),TeC16, the line shape is observed to relax isotropically, implying that continuous C3 rotations are taking place. Les couplages entre sommets qui ont etC mesurCes sont plus faibles que ceux que l'on peut prCdire sur la base du mouvement C3 autour de l'axe de symCtrie molCculaire. I1 est possible de crCer un modkle de la forme de ces raies en faisant I'hypothkse que les rotations C3 des groupes methyle et ammonium se produisent alors que l'axe C-N est en libration dans un cBne effectif autour de la position de l'axe molCculaire statique. Pour les sels (CH3ND3),TeBr6 et (CD3NH3)TeBr6, on a mesurk les couplages entre somrnets dans les spectres Rh4N du 'H, dCterminCs en fonction de la tem+rature, pour les phases 11, III et IV; on a trouvC qu'ils sont semblables....