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Bifurcated Hydrogen Bonding and Asymmetric Fluctuations in aCarbohydrate Crystal Studied via X-ray Crystallography and Computationalanalysis

机译:氢的分叉氢键和不对称涨落通过X射线晶体学和计算研究的碳水化合物晶体分析

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摘要

The structure of the O-methyl glycoside of the naturally occurring 6-O-[(R)-1-carboxyethyl]-α-d-galactopyranose, C10H18O8, has been determined by X-ray crystallography at 100 K, supplementing the previously determined structure obtained at 293 K (Acta Cryst., 1996, C52, 2285-2287). Molecular dynamics simulations of this glycoside were performed in the crystal environment with different numbers of units cells included in the primary simulation system at both 100 K and 293 K. The calculated unit cell parameters and the intra-molecular geometries (bonds, angles, and dihedrals) agree well with experimental results. Atomic fluctuations, including B-factors and anisotropies, are in good agreement with respect to the relative values on an atom-by-atom basis. In addition, the fluctuations increase with increasing simulation system size, with the simulated values converging to values lower than those observed experimentally indicating that the simulation model is not accounting for all possible contributions to the experimentally observed B-factors which may be related to either the simulation time scale or size. In the simulations thehydroxyl group of O7 is found to form bifurcated hydrogen bonds with O6 and O8of an adjacent molecule, with the interactions dominated by the HO7-O6interaction. Quantum mechanical calculations support this observation.
机译:天然存在的6-O-[(R)-1-羧乙基]-α-d-吡喃半乳糖C10H18O8的O-甲基糖苷的结构已通过X射线晶体学在100 K下测定,补充了先前确定的结构在293 K时获得(Acta Cryst。,1996,C52,2285-2287)。该糖苷的分子动力学模拟是在晶体环境中以100 K和293 K在主模拟系统中使用不同数量的晶胞进行的。计算的晶胞参数和分子内几何结构(键,角和二面体) )与实验结果非常吻合。原子波动,包括​​B因子和各向异性,相对于每个原子的相对值而言,是非常一致的。此外,波动随着模拟系统规模的增加而增加,模拟值收敛到低于实验观察到的值,这表明模拟模型并未考虑到对实验观察到的B因子的所有可能贡献,而B因子可能与两个模拟的时间尺度或大小。在模拟中发现O7的羟基与O6和O8形成分叉的氢键分子的相互作用,其相互作用主要由HO7-O6决定相互作用。量子力学计算支持这一观察。

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