1,6-无水-β- d -葡萄糖在塑料晶体、取向玻璃、液体和普通玻璃中的结构:分子建模和x射线衍射研究

K. Jurkiewicz, Wojciech Glajcar, K. Kamiński, L. Temleitner, A. Burian
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引用次数: 1

摘要

利用x射线衍射和分子模型研究了1,6-无水-β- d -葡萄糖醛酸(左旋葡聚糖)的塑料晶体(PC)、取向玻璃(OTG)、液相(LQ)和普通玻璃(OG)相的结构。以静态结构因子和对分布函数的形式对实验衍射数据在倒数空间和实空间进行了分析,并与基于模型的模拟结果进行了比较。采用了一种新的方法来模拟无序相的结构,该方法考虑了以尖锐布拉格峰形式出现的分子间散射贡献、与分子内相关性相关的缓慢变化强度以及由结构无序引起的扩散成分。在LQ和OG样本的情况下,反向蒙特卡罗模拟也被使用。PC相和OTG相表现出六方密排(hcp)型结构的长程有序,最高可达120 Å,分子取向随机。假设分子骨架是刚性的,在该结构的理论模型中产生了分子围绕其几何中心在完全和有限角度范围内的各向同性自由旋转。结果表明,采用分子的自由旋转导致左旋葡聚糖的每个研究相的实验数据的最佳拟合。LQ和OG样品的衍射图显示出一个相对尖锐的第一峰,它来自于密集排列的面心立方(fcc)型分子排列的准布拉格面。此外,LQ和OG的缓变强度组分与PC和OTG的缓变强度组分基本相同,说明这四相的分子内结构没有发生变化。有趣的是,无序LQ和OG状态的结构相关性出奇地远,高达约50 Å。此外,在所研究的所有左旋葡聚糖相中,对生成的模型施加的准晶无序性导致与实验数据的一致性更好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Structure of 1,6-anhydro-β-D-glucopyranose in plastic crystal, orientational glass, liquid and ordinary glass forms: molecular modeling and X-ray diffraction studies
The structures of the plastic crystal (PC), orientational glass (OTG), liquid (LQ) and ordinary glass (OG) phases of 1,6-anhydro-β-D-glucopyranose (levoglucosan) have been investigated using X-ray diffraction and molecular modeling. The experimental diffraction data in the forms of static structure factors and pair distribution functions are analyzed in reciprocal and real spaces and compared with results of model-based simulations. A new approach to modeling the structure of the disordered phases, taking into account the intermolecular scattering contribution in the form of sharp Bragg peaks, the slowly varying intensity associated with intramolecular correlations and the diffusive component resulting from structural disorder, is applied. In the case of the LQ and OG samples, reverse Monte Carlo simulations are also used. The PC and OTG phases show long-range ordering of the hexagonal close-packed (hcp)-type structure up to 120 Å with random orientation of the molecules. Assuming a rigid molecular skeleton, isotropic free rotations of the molecules about their geometrical center in full and limited angular ranges are generated in theoretical models of the structure. It is demonstrated that the adoption of free rotations of the molecules leads to the best fits to experimental data for each studied phase of levoglucosan. The diffraction patterns of the LQ and OG samples show a relatively sharp first peak originating from quasi-Bragg planes of the densely packed face-centered cubic (fcc) type molecular arrangement. Moreover, the slowly varied intensity component of LQ and OG is practically the same as that of PC and OTG, suggesting that the intramolecular structure of these four phases does not change. Interestingly, structural correlations for the disordered LQ and OG states extend surprisingly far, up to about 50 Å. In addition, for all levoglucosan phases investigated, the paracrystalline disorder imposed on the generated models resulted in better compliance with the experimental data.
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