Abstract

Carbon-13 spin-lattice relaxation times and nuclear Overhauser enhancements of dichloromethane were measured in “inert” solvents of varying viscosity and in various Lewis basic solvents. Derived CH rotational correlation times were observed to remain approximately constant in the non-interactive mixtures, but to increase, by as much as a factor of three, in the basic solvents. Correlation times calculated by the Hu-Zwanzig slip model were, in all cases, shorter than the measured values. The theory predicted a viscosity dependence of τ c , which was not observed experimentally. Rotational times calculated with the Hynes-Kapral-Weinberg model were somewhat longer than the observed values. However, the theory did correctly predict that τ c should be approximately independent of viscosity in the non-interactive mixtures. A close agreement between theory and experiment was found for dichloromethane in the basic solvents. Therefore, the increase of τ c in these solutions cannot be ascribed to slowed reorientation of the associated dimer. The results suggest that the CH bond retains a degree of rotational mobility in the hydrogen bonded complex.

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