Celebre Giorgio, Concistré Maria, De Luca Giuseppina, Longeri Marcello, Pileio Giuseppe
Universitá della Calabria, Dipartimento di Chimica Via P. Bucci, 87030 Arcavacata di Rende (Cs), Italy.
Chemphyschem. 2006 Sep 11;7(9):1930-43. doi: 10.1002/cphc.200600220.
The conformational equilibrium of 1,3-butadiene in a condensed fluid phase is investigated by liquid-crystal NMR spectroscopy. The full set of D(HH) and D(CH) dipolar couplings is determined from the analysis of the (1)H spectra of the three 1,3-butadiene most-abundant isotopomers (i.e. the all (12)C and the two single-labeled (13)C isotopomers) for a total of 21 independent dipolar couplings. A very good starting set of spectral parameters for the analysis of the (1)H spectrum is determined in a semiautomated way by the analysis of the (N-1) (specifically, N=6, the number of 1/2 spin nuclei in the spin system) quantum refocused (5QR), and not (5Q), spectra. As an alternative approach, a Monte Carlo (MC) numerical simulation, capable of predicting the solute ordering, is tested to simulate the 5QR spectrum. The set of D(ij) couplings is very good, proving that the MC method can represent a novel, valid alternative to the existing spectral simplification procedures. The experimentally determined dipolar-coupling data set is fully compatible with the 1,3-butadiene conformational distribution reported in the literature for isolated molecules, indicating the presence of about 99 % of s-trans conformer. With regards to the remaining 1 %, in spite of the direct and very strong dependence of the observables on the molecular structure, it was not possible to discriminate between the planar s-cis and s-gauche forms, both of which produce a very good fit of the dipolar couplings. Vibrational corrections, up to the anharmonic term, were applied; the calculated geometrical parameters are in good- although not exact-agreement with those reported in the literature from experimental and theoretical investigations. This result can be considered as supporting the methodology used for obtaining the structure and conformational distribution of a flexible molecule in a liquid phase.
采用液晶核磁共振光谱法研究了1,3 - 丁二烯在凝聚流体相中的构象平衡。通过分析三种1,3 - 丁二烯最丰富的同位素异构体(即全(12)C和两种单标记(13)C同位素异构体)的(1)H谱,确定了完整的D(HH)和D(CH)偶极耦合,总共得到21个独立的偶极耦合。通过对(N - 1)(具体来说,N = 6,自旋系统中1/2自旋核的数量)量子重聚焦(5QR)而非(5Q)谱的分析,以半自动方式确定了用于分析(1)H谱的一组非常好的光谱参数。作为一种替代方法,测试了一种能够预测溶质有序性的蒙特卡罗(MC)数值模拟,以模拟5QR谱。D(ij)耦合集非常好,证明MC方法可以成为现有光谱简化程序的一种新颖、有效的替代方法。实验测定的偶极耦合数据集与文献中报道的孤立分子的1,3 - 丁二烯构象分布完全兼容,表明存在约99%的s - 反式构象体。关于其余的1%,尽管观测值与分子结构有直接且非常强的依赖性,但无法区分平面s - 顺式和s - gauche形式,这两种形式都能很好地拟合偶极耦合。应用了直至非谐项的振动校正;计算得到的几何参数与文献中通过实验和理论研究报道的参数吻合良好,尽管并不完全精确。这一结果可被视为支持用于获得液相中柔性分子结构和构象分布的方法。