Borisenko Konstantin B, Rankin David W H
School of Chemistry, University of Edinburgh, West Mains Road, Edinburgh KEH9 3JJ, UK.
Dalton Trans. 2005 Jul 21(14):2382-7. doi: 10.1039/b504275e. Epub 2005 Jun 9.
Quantum chemical calculations of the structures and thermodynamics of homolytic dissociation of the central P-P and N-N bonds in tetrakis(disyl)diphosphine and tetrakis(di-tert-butylsilyl)hydrazine have been performed. The theory predicted negative standard enthalpies for homolytic bond dissociation in both cases, -71.0 and -108.4 kJ mol(-1) for the diphosphine and hydrazine, respectively, using the ONIOM (MP2/6-31+G*:B3LYP/3-21G*) level. The dissociation is accompanied by considerable structural changes in the radicals as compared to the corresponding fragments of the parent molecules, resulting in low dissociation enthalpies. The most pronounced changes in both radicals are the relaxation of bond angles in the substituents and a conformational change in the orientation of the substituent groups. In addition, the bis(di-tert-butylsilyl)aminyl radical displays a considerable increase in Si-N-Si angle and shortening of the Si-N bonds upon dissociation. These changes are not associated with any appreciable delocalisation of the lone electron, as the spin density is found from the B3LYP/3-21G* calculations to be largely concentrated on the nitrogen atom. It has been also shown that although the dissociation energies are low for both compounds, the intrinsic energies of the central bonds are still high, 140.6 kJ mol(-1) for the P-P bond in tetrakis(disyl)diphosphine and 490.6 kJ mol(-1) for the N-N bond in tetrakis(di-tert-butylsilyl)hydrazine, using the ONIOM method. The calculations predict that the dissociation of tetrakis(disyl)diphosphine would have negative free energy even without taking relaxation of the fragments into account, while the full potential of releasing about 306 kJ mol(-1) of energy stored in the ligands of tetrakis(di-tert-butylsilyl)hydrazine is only fully realised upon a considerable separation of the fragments.
已对四(二硅基)二膦和四(二叔丁基硅基)肼中中心P-P键和N-N键的均裂解离结构及热力学进行了量子化学计算。理论预测,在这两种情况下均裂键解离的标准焓为负值,使用ONIOM(MP2/6-31+G*:B3LYP/3-21G*)水平计算,二膦和肼的分别为-71.0和-108.4 kJ mol⁻¹。与母体分子的相应片段相比,解离伴随着自由基中显著的结构变化,导致解离焓较低。两种自由基中最明显的变化是取代基中键角的松弛以及取代基基团取向的构象变化。此外,双(二叔丁基硅基)氨基自由基在解离时Si-N-Si角显著增大且Si-N键缩短。这些变化与孤电子的任何明显离域无关,因为从B3LYP/3-21G*计算发现自旋密度主要集中在氮原子上。还表明,尽管两种化合物的解离能都很低,但使用ONIOM方法计算,四(二硅基)二膦中P-P键的本征能仍很高,为140.6 kJ mol⁻¹,四(二叔丁基硅基)肼中N-N键的本征能为490.6 kJ mol⁻¹。计算预测,即使不考虑片段的松弛,四(二硅基)二膦的解离也会有负的自由能,而四(二叔丁基硅基)肼配体中储存的约306 kJ mol⁻¹能量的全部潜力只有在片段充分分离时才会完全实现。