Jr. Polam et al., RATES OF AXIAL LIGAND ROTATION IN DIAMAGNETIC D(6) CO(III) AND FE(II)PORPHYRINATES, Inorganica Chimica Acta, 263(1-2), 1997, pp. 109-117
In order to investigate the rates of rotation of pyridine and imidazol
e ligands in diamagnetic low-spin d(6) Co(III) and Fe(II) porphyrinate
systems, we have synthesized tetramesitylporphyrinate (TMP) complexes
of each of these metals with pyridine and imidazole ligands and inves
tigated them as a function of temperature by LH NMR spectroscopy. We h
ave already reported that for TMPFe(III) and -Co(III) complexes with h
indered imidazoles the TMP o-CH3 resonances can be used to measure the
rates of rotation (N.V Shokhirev, T.Kh. Shokhireva, J.R. Polam, C.T.
Watson, K. Raffii, U. Simonis and F.A. Walker, J. Phys. Chern. A, 101
(1997) 2778). For the bis-1,2-dimethylimidazole complex, [TMPCo(1,2-Me
(2)Im)(2)] BF4, at ambient temperatures ligand rotation is slow but me
asureable on the NMR time scale, and four o-CH3 resonances are observe
d, as we have already reported. In contrast, as shown in the present w
ork, for the bis-4-dimethylaminopyridine complex, [TMPCo(4-NMe2Py)(2)]
BF4, ligand rotation is extremely rapid at ambient temperatures. At t
emperatures below -50 degrees C at 300 MHz the o-CH, resonance broaden
s and the rates of rotation can be estimated using the modified Bloch
equations simplified for the fast exchange regime. The activation para
meters Delta H-not equal and Delta S-not equal have been determined, a
nd the extrapolated rate constant at 25 degrees C, k(ex) greater than
or equal to 1.1 x 10(6) s(-1). These results contradict previous repor
ts (J. Huet and A. Gaudemer, Org. Magn. Reson., 15 (1981) 347; I. Cass
idei, H. Bang, J.O. Edwards and R. G. Lawler, J. Phys. Chem., 95 (1991
) 7186) that pyridine ligands bound to Co(III) porphyrinates do not ro
tate at room temperature in homogeneous solution. For unhindered imida
zole complexes, such as [TMPCo(NMeIm)(2)]+BF4-, no broadening of the o
-CH3 resonance is observed, even at -90 degrees C, and thus the rate o
f axial ligand rotation is too fast to measure, even at that low tempe
rature (or the difference in chemical shift of the two resonances expe
cted if ligand rotation is slow is very small). For the corresponding
Fe(II) porphyrinate complexes, the rates of pyridine and unhindered im
idazole rotation are too fast to measure, even at -90 degrees C. The 2
-methylimidazole complex undergoes chemical reactions that prevent det
ailed study of this system by NMR spectroscopy, but the 1,2-dimethylim
idazole complex is stable and of similar structure (ruffled porphyrina
te ring, axial ligands in perpendicular planes) to the Co(III) and Fe(
III) analogs, with the rate constant for ligand rotation, k(ex) simila
r to 1 s(-1), at -90 degrees C. Assuming a similar activation enthalpy
to those of the Co(III) and Fe(III) systems, the rate of rotation of
axial ligands in [TMPFe(1,2-Me(2)Im)(2)] at 25 degrees C is estimated
to be about 2 x 10(4) s(-1). (C) 1997 Elsevier Science S.A.