Jp. Charland et al., BINDING OF THE LOPSIDED 1,5,6-TRIMETHYLBENZIMIDAZOLE LIGAND TO INORGANIC AND ORGANOMETALLIC COBALOXIME B-12 MODELS, Inorganic chemistry, 32(20), 1993, pp. 4256-4267
The interaction of the lopsided dimethylbenzimidazole ligand with the
corrin ligand in cobalamins (Cbls) may be one of the structural featur
es involved in Co-C bond cleavage during B-12-dependent enzymic proces
ses. Models of B-12 compounds usually contain alkyl ligands to mimic t
he coenzymes. However, the inductive effect of the Co on the benzimida
zole ligand should be most pronounced when the trans influence of the
other axial ligand is weak, e.g. Cl. In this report we describe the sy
nthesis and three-dimensional structures of Me3BzmnCo(DH)2Cl (I) and s
everal alkylcobaloximes, Me3BzmCo(DH)2R(where Me3Bzm = 1,5,6-trimethyl
benzimidazole,DH = the monoanion of dimethylglyoxime, and R = CH2NO2 (
II), R = CH3 (III), and CH(CH3)2 (IV)). The X-ray results suggest that
this benzimidazole ligand does not have unusual bulk and closely rese
mbles pyridine in steric effect. The geometry at the Co-coordinated N
of Me3Bzm is characterized by large angular distortions. However, the
distortions were not very dependent on the trans ligand. A two-term ex
pression has been reported previously to explain the dependence of the
C-13 NMR chemical shifts for the alpha-ribazole (dimethylbenzimidazol
e-containing) moiety in Cbls on changes in the trans axial ligand. The
first (through-bond) inductive term relates the inductive effect of t
he cobalt center to that of the proton. The second (through-space) ani
sotropic term relates the effects of changes in structure and cobalt a
nisotropy on chemical shift. We attempted to use an analogous expressi
on to fit our structural and NMR data on Me3Bzm cobaloximes with trans
ligands of greatly different trans influence. The proton inductive ef
fects were not useful for explaining the cobalt inductive effects, sin
ce the C-13 NMR signal for B2 (the C between the two benzimidazole N's
) moved down field on coordination in our models but upfield on coordi
nation in Cbls. Protonation causes the B2 signal to move upfield. Ther
efore, with our extensive data, we developed a new empirical inductive
term which gave excellent fits of our data, expressed as coordination
shifts. Coordination shifts are the differences in shift of the free
and coordinated ligand. The possible significance of this new term is
discussed in the tight of the finding that it gave values consistent w
ith the effects of other metal ions on the B2 coordination shifts and
with other measures of the influence of axial ligands on the propertie
s of the cobalt center. Furthermore, the upfield coordination shift of
B2 in Cbls can now be confidently attributed to corrin ring anisotrop
y; the shift is only slightly modulated by cobalt inductive and anisot
ropic effects. Moreover, the small dependence of the B2 shift on the t
rans influence of the other axial ligand (the ligand-responsive shift)
cannot be rationalized with the published two-term proton-based expre
ssion. With our new interpretation, a consistent description of ligand
-responsive shifts emerges for both Cbls and B-12 models. Finally, our
reinterpretation of factors influencing C-13 NMR shifts also accounts
for some significant features of the IH NMR spectra of Cbls.