Information about 14N relaxation times and (N, F) coupling constants is obtained for three fluoropyridines from (a) a detailed band-shape analysis of the broad 19F resonance bands assigned to ortho-fluorine nuclei, (b) 14N resonance bands, and (c) 15N satellites in 19F resonance. The effects of medium and of temperature were investigated, and activation energies for rotational diffusion are given. Double resonance experiments show that the meta (F, F) coupling constants for 3-chloro-2,4,5,6-tetrafluoropyridine vary in sign.
INTRODUCTIONIndirect scalar spin-spin coupling constants between nuclei of spin-89 have become the subject of a vast and expanding literature. However, few studies of coupling constants involving nuclei of spin greater than 89 have been reported, since such nuclei are usually rapidly relaxed by the interaction of their electric quadrupole moments with the fluctuating electric field gradients resulting from molecular re-orientation. Nuclei with large quadrupole moments are relaxed so effectively by this mechanism that they usually produce no observable effects in the spectrum of a spin-89 nucleus in the same molecule. A few coupling constants involving a quadrupolar nucleus have been measured directly in cases where the electric field gradient is zero by symmetry [1-4], or where the field gradient is small, as for isocyanides [5][6][7][8]. For such systems the spin-lattice relaxation time of the quadrupolar nucleus (T1A) can be obtained simply from measurement of the halfwidths of the components of the resonance of the spin-89 nuclei [9,10]. For rates of relaxation so rapid that the resonance of a magnetically equivalent group of spin-89 nuclei (X) in the same molecule is a single line (other spin-~ nuclei being absent), the coupling constant (JAx) can be measured [11,12] by studying the field dependence of the spin-lattice (Tlx) and spin-spin (T2x) relaxation times of the X nuclei. The theoretical basis of the method lies in the fact that under these fast exchange conditions the scalar coupling has become a relaxation mechanism of the second kind [10] for the X nuclei. In practice the field dependence of the relaxation time is only detectable when