Abstract
Ab initio calculations have been carried out on MR2 complexes (where M = Pd or Pt and R = H or CH3) to model concerted reductive coupling from MR2L2 complexes (where L is a substituted phosphine). The results of these calculations support the following two conclusions. (1) The difference in the driving force for reductive elimination from Pd(II) and Pt(II) complexes with the same R groups is very close (0–4 kcal/mol) to the difference in the s1d9-d10 state splittings of these elements (32 kcal/mol). Thus reductive elimination is exothermic from Pd complexes (since Pd prefers d10) and endothermic from Pt complexes (since Pt prefers s1d9), where the metal product is in its d10 state. This supports the conclusion, derived from qualitative considerations of generalized Valence bond wave functions, that Pt(II) and Pd(II) complexes have their metal atoms in an s1d9 configuration and the metal atoms in Pt(0) and Pd(0) complexes are in a d10 configuration. (2) The activation Barriers for C-C coupling are approximately twice that for C-H coupling. There are Essentially no Barriers for processes involving H-H bonds. The origin of this trend is the directionality of the methyl sp3 orbital, which destabilizes the transition state for the case where an M-C bond is being converted to a C-C or C-H bond. Conversely, the spherical H 1s orbital can form multicenter bonds easily, allowing it to break M-H bonds while forming an H-H bond and leading to low intrinsic Barriers. These results are consistent with the experimentally observed trends.
| Original language | English |
|---|---|
| Pages (from-to) | 609-622 |
| Number of pages | 14 |
| Journal | Organometallics |
| Volume | 5 |
| Issue number | 4 |
| DOIs | |
| Publication status | Published - 1 Jan 1986 |
| Externally published | Yes |
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