The complexes [Fe(Cp)(SnPh3)(CO)(PR3)] (PR3 = PMe3 (1), PnBu3 (2), PCy3 (3), PMe2Ph (4), PMePh2 (5), P(CH2Ph)3 (6), PPh3 (7), P(4-MeC6H4)3 (8),
P(4-MeOC6H4)3 (9), P(4-FC6H4)3 (10), P(4-CF3C6H4)3 (11), P(NMe2)3 (12), P(OMe)3 (13), P(OPh)3 (14)), which have been
characterized by X-ray crystallography (except for 1 and 4), infrared spectroscopy (carbonyl stretching frequency,
νCO), and NMR spectroscopy (13C, 31P, 57Fe, 119Sn) offer some insight
into the response of the iron nucleus to changes in the electronic
and steric properties of the PR3 ligand. A fairly good
correlation is found between the 57Fe chemical shift and
the Tolman cone angle θ for PR3 and a rather poorer
correlation between δ(57Fe) and νCO. However, for the subseries of complexes 7–11 having PR3 = P(4-XC6H4)3 (X = H, Me, MeO, F, CF3), the correlation
between δ(57Fe) and νCO is very
good. Since the steric properties of these ligands, from the point
of view of the metal, are identical (θ = 145°), this provides
a means of separating the steric and electronic contributions of PR3 to δ(57Fe). The electronic contribution
of PR3 to δ(57Fe) can be further separated
into σ and π components by making use of the finding that
the π component of the Fe–P bond has a negligible influence
on δ(57Fe), unlike its influence on νCO. The ligands PMe3, PnBu3, PCy3, PMe2Ph, PMePh2, and P(NMe2)3 are found to be “pure” σ donors,
P(OMe)3 and P(OPh)3 are found to be π
acceptors of differing strength, and P(4-XC6H4)3 is found to show weak but clearly distinguishable π
acceptor properties.