Güizado-Rodríguez M, Ariza-Castolo A, Merino G, Vela A, Noth H, Bakhmutov V I, Contreras R
Departamento de Química, Centro de Investigación y de Estudios Avanzados, A.P. 14-740, C.P. 07000, México D.F, México.
J Am Chem Soc. 2001 Sep 19;123(37):9144-52. doi: 10.1021/ja0111232.
Bis(NBH(3)), bis(NBF(3)), and NBF(3)/NBH(3) adducts 1-3 were prepared from 1,3-dimethyl-1,3-diazolidine and characterized by the (1)H, (13)C, (11)B, (19)F, 2D (1)H(-13)C HETCOR and NOESY NMR spectra. The structures and conformations of the adducts were established by the variable-temperature (1)H NMR spectra, the X-ray diffraction method (adduct 2A), and density functional calculations at different theoretical levels. The experimental and theoretical data have revealed that bis adducts 1-3 prefer trans orientations of the borane groups (1A, 2A, 3A) in solution, the solid state, and the gas phase. The studies have shown that the energetic preference of trans adducts with respect to cis compounds, decreasing as 2A (2.9 kcal/mol) > 3A (2.7 kcal/mol) > 1A (1.4 kcal/mol), is dictated by spatially repulsive interactions between the CH(3), BH(3), and BF(3) groups. The results of DFT calculations agree well with an experimental trans/cis isomeric ratio of 9:1 determined in solutions of adduct 1. The calculated geometry and energy, as well as the topological analysis of electronic densities, show that trans adducts 1-3 should exist in gas phase as twist conformations T-2 stabilized by the intramolecular C-H(delta+)...(-delta)H-B or C-H(delta+)...(-delta)F-B interactions. These interactions are characterized as closed-shell. The energy of one proton-hydride and proton-fluoride intramolecular contact, estimated as 1.9 (1A-T-2) and 0.7 (2A-T-2) kcal/mol, respectively, classifies the "elongated" intramolecular interactions CH(delta+)...(-delta)HB and CH(delta+)...(-delta)FB as weak ones. It has been established that, on going from gas phase to a condensed phase (solution and solid), the twist-conformations T-2 transform to conformations T-1, probably by intermolecular dipole-dipole interactions. The data presented in this work show that despite a weakness of the "elongated" proton-hydride and proton-fluoride interactions, they can play a significant role in the stabilization of conformational molecular states, especially when cooperativity is in action.
双(硼氢化氮)、双(三氟化硼氮)以及三氟化硼氮/硼氢化氮加合物1 - 3由1,3 - 二甲基 - 1,3 - 二氮杂环戊烷制备而成,并通过氢谱(¹H)、碳谱(¹³C)、硼谱(¹¹B)、氟谱(¹⁹F)、二维¹H - ¹³C异核多量子相干谱(HETCOR)和核Overhauser效应谱(NOESY)核磁共振谱进行表征。通过变温¹H核磁共振谱、X射线衍射法(加合物2A)以及不同理论水平的密度泛函计算确定了加合物的结构和构象。实验和理论数据表明,双加合物1 - 3在溶液、固态和气态中硼烷基团更倾向于反式取向(1A、2A、3A)。研究表明,反式加合物相对于顺式化合物的能量优势按2A(2.9千卡/摩尔)> 3A(2.7千卡/摩尔)> 1A(1.4千卡/摩尔)的顺序递减,这是由甲基、硼氢化氢和三氟化硼基团之间的空间排斥相互作用决定的。密度泛函理论(DFT)计算结果与在加合物1的溶液中测定的9:1的反式/顺式异构体比例吻合良好。计算得到的几何结构和能量,以及电子密度的拓扑分析表明,反式加合物1 - 3在气相中应以通过分子内C - H(δ⁺)...(-δ)H - B或C - H(δ⁺)...(-δ)F - B相互作用稳定的扭曲构象T - 2存在。这些相互作用的特征为闭壳层。一个质子 - 氢化物和质子 - 氟化物分子内接触的能量分别估计为1.9(1A - T - 2)和0.7(2A - T - 2)千卡/摩尔,这将“拉长的”分子内相互作用CH(δ⁺)...(-δ)HB和CH(δ⁺)...(-δ)FB归类为弱相互作用。已经确定,从气相到凝聚相(溶液和固态),扭曲构象T - 2可能通过分子间偶极 - 偶极相互作用转变为构象T - 1。这项工作中呈现的数据表明,尽管“拉长的”质子 - 氢化物和质子 - 氟化物相互作用较弱,但它们在构象分子态的稳定中可以发挥重要作用,特别是当协同作用起作用时。