Theoretical study of the structure, bonding nature, and reductive elimination reaction of Pd(XH3)(eta(3)-C3H5) (PH3) (X = C, Si, Ge, Sn). Hypervalentbehavior of group 14 elements
B. Biswas et al., Theoretical study of the structure, bonding nature, and reductive elimination reaction of Pd(XH3)(eta(3)-C3H5) (PH3) (X = C, Si, Ge, Sn). Hypervalentbehavior of group 14 elements, ORGANOMETAL, 18(20), 1999, pp. 4015-4026
The structure and bonding nature of Pd(XH3)(eta(3)-C3H5)(PH3) (R-X; X = C,
Si, Ge, Sn) and its C-X reductive elimination were investigated with MP2-MP
4(SDQ) and CCSD(T) methods. The C-C reductive elimination is considerably e
xothermic (27.7 kcal/mol) and needs a significantly large activation energy
(23.0 kcal/mol), where CCSD(T) values are given hereafter. This considerab
ly large exothermicity can be easily interpreted in terms of the strong C-C
bond and the weak Pd-CH3 bond. On the other hand, the C-Si, C-Ge, and C-Sn
reductive eliminations easily occur with a moderate activation barrier (12
-13 kcal/mol) and a moderate reaction energy; the exothermicities are 6.0 a
nd 1.6 kcal/mol for the C-Si and C-Ge reductive eliminations, respectively,
and the endothermicity of the C-Sn reductive elimination is 6.0 kcal/mol.
These moderate reaction energies of C-Si, C-Ge, and C-Sn reductive eliminat
ions are interpreted in terms of the decreasing orders of bond energy E(C-C
) > E(C-Si) > E(C-Ge) > E(C-Sn) and E(Pd-SiH3) > E(Pd-GeH3) > E(Pd-SnH3) mu
ch greater than E(Pd-CH3). The moderate activation barriers of C-Si, C-Ge,
and C-Sn reductive eliminations are reflected in their transition state str
uctures, in which SiH3, GeH3, and SnH3 groups can interact with the allyl c
arbon atom, keeping the Pd-SiH3, Pd-GeH3, and Pd-SnH3 bonds intact. These f
eatures result from the hypervalency of these elements. In the C-C reductiv
e elimination, the Pd-CH3 bond considerably weakens but the allyl-CH3 bond
is not completely formed at the TS, which is consistent with no hypervalenc
y of the C atom. The eta(1)-allyl form, Pd(XH3)(eta(1)-C3H5)(PH3), is much
less stable than R-X by 7-8 kcal/mol. Intrinsic reaction coordinate calcula
tions clearly show that the C-C reductive elimination occurs not through th
e eta(1)-allyl form but directly from Pd(CH3)(eta(3)-C3H5)(PH3) if PH3 does
not exist in excess. If excess PH3 exists in the reaction medium, the C-X
reductive elimination via Pd(XH3)(eta(1)-C3H5)(PH3)(2) is not excluded. The
(eta(3)-C3H5)-XH3 (X = C, Sn) reductive elimination requires a larger acti
vation energy than the CH3-XH3 reductive elimination, because the Pd-(eta(3
)-C3H5) bond is stronger than the Pd-CH3 bond.