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

Citation
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
Citations number
60
Categorie Soggetti
Organic Chemistry/Polymer Science
Journal title
ORGANOMETALLICS
ISSN journal
02767333 → ACNP
Volume
18
Issue
20
Year of publication
1999
Pages
4015 - 4026
Database
ISI
SICI code
0276-7333(19990927)18:20<4015:TSOTSB>2.0.ZU;2-8
Abstract
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.