Gronert Scott, Keeffe James R
Department of Chemistry and Biochemistry, San Francisco State University, 1600 Holloway Avenue, San Francisco, California 94132, USA.
J Am Chem Soc. 2005 Feb 23;127(7):2324-33. doi: 10.1021/ja044002l.
Enthalpies of addition of hydride ion to eleven carbonyl acceptors (X-CHO), two conjugate addition sites (X-CH=CH2; X = CHO, NO2), eight carbenium ion acceptors, fulvene, borane, and SiH3(+) were calculated at the MP2/6-311+G level. Correlation between calculated and experimental enthalpies of addition of hydride ion is excellent. Transition states (ts) for the identity hydride transfers between the acceptors and their corresponding hydride adducts (hydride donors) were also calculated. The carbonyl and fulvene reactions have transition states with one imaginary frequency: the hydrogen transfer coordinate. The carbenium ions, borane, and SiH3(+) gave not transition states but stable compounds upon addition of the hydride donor. Computational differences between these hydride transfers and previously reported proton transfers include shorter partial C...H bonds and a tendency toward bent C...H...C angles for the hydride transfer ts and addition compound structures, particularly when a bent geometry improves interactions elsewhere in the structure. These and other differences are explained by modeling the hydride transfer ts and addition compounds as two-electron, three-center systems involving the transfer termini and the shared hydrogen but the proton transfer ts structures as four-electron, three-center systems. Charge and geometry measures suggest transition states in which these features change synchronously, again in contrast to many proton transfer reactions. For the X-CHO set, polar effects dominate enthalpies of hydride addition, with resonance effects also important for resonance donors; these preferentially stabilize the acceptor, reducing its hydride ion affinity. Activation enthalpies are dominated by resonance stabilization of the acceptors, greatly attenuated in the transition states.
在MP2/6 - 311+G水平下计算了氢负离子加成到11种羰基受体(X - CHO)、2个共轭加成位点(X - CH=CH₂;X = CHO、NO₂)、8种碳正离子受体、富烯、硼烷和SiH₃⁺上的焓变。计算得到的氢负离子加成焓与实验值之间的相关性极佳。还计算了受体与其相应氢化物加合物(氢化物供体)之间氢负离子转移的过渡态(ts)。羰基和富烯反应的过渡态具有一个虚频:氢转移坐标。碳正离子、硼烷和SiH₃⁺在加入氢化物供体后没有给出过渡态,而是得到了稳定的化合物。这些氢负离子转移与先前报道的质子转移之间的计算差异包括较短的部分C...H键以及氢负离子转移过渡态和加合物结构中C...H...C角呈弯曲趋势,特别是当弯曲几何结构改善了结构中其他位置的相互作用时。通过将氢负离子转移过渡态和加合物建模为涉及转移端和共享氢的双电子三中心体系,而将质子转移过渡态结构建模为四电子三中心体系,可以解释这些差异及其他差异。电荷和几何测量表明过渡态中这些特征同步变化,这再次与许多质子转移反应形成对比。对于X - CHO组,极性效应主导氢负离子加成焓,共振效应对于共振供体也很重要;这些效应优先稳定受体,降低其对氢负离子的亲和力。活化焓由受体的共振稳定作用主导,在过渡态中大大减弱。