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核磁共振、分子模拟和流体动力学在三糖构象分析中的应用。

Application of NMR, molecular simulation, and hydrodynamics to conformational analysis of trisaccharides.

作者信息

Dixon Ann M, Venable Richard, Widmalm Göran, Bull T E, Pastor Richard W

机构信息

Laboratory of Biophysics, Center for Biologics Evaluation and Research, Food and Drug Administration, 1401 Rockville Pike, Rockville, MD 20852-1448, USA.

出版信息

Biopolymers. 2003 Aug;69(4):448-60. doi: 10.1002/bip.10421.

Abstract

The preferred conformations and conformational flexibilities of the trisaccharides alpha-D-Glcp-(1-->2)-beta-D-Glcp-(1-->3)-alpha-D-Glcp-OMe (I) and alpha-D-Glcp-(1-->3)[beta-D-Glcp-(1-->4)]-alpha-D-Glcp-OMe (II) in aqueous solution were determined using nuclear magnetic resonance (NMR) spectroscopy, molecular dynamics (MD) and Langevin dynamics (LD) simulations, and hydrodynamics calculations. Both trisaccharides have a vicinal substitution pattern in which long range (nonsequential) interactions may play an important role. LD simulation at 600 K indicated that the all-syn conformation predominated, though other conformations were apparent. NOE data and MD and LD simulations at 298 K all indicated that trisaccharide I is a single all-syn conformer in solution. Given that previous studies showed evidence of anti-conformers in beta-D-Glcp-(1-->2)-beta-D-Glcp-(1-->3)-alpha-D-Glcp-OMe, this result provides an example of how changing the anomeric configuration of one residue from beta to alpha can make an oligosaccharide more rigid. Discrepancies in inter-ring distances obtained by experiment and by simulation of the all-syn conformer suggest the presence of an anti-psi conformation at the beta-(1-->4)-linkage for II. A combined analysis of measured and calculated translational diffusion constants and (13)C T(1) relaxation times yield order parameters of 0.9 for each trisaccharide. This implies that any interconversion among conformations is significantly slower than tumbling. Anisotropies of approximately 1.6 and 1.3 calculated for I and II, respectively, are consistent with the observed relatively flat T(1) profiles because the tumbling is not in the motional narrowing regime.

摘要

利用核磁共振(NMR)光谱、分子动力学(MD)和朗之万动力学(LD)模拟以及流体动力学计算,确定了三糖α-D-葡萄糖吡喃糖基-(1→2)-β-D-葡萄糖吡喃糖基-(1→3)-α-D-葡萄糖吡喃糖基-OMe(I)和α-D-葡萄糖吡喃糖基-(1→3)[β-D-葡萄糖吡喃糖基-(1→4)]-α-D-葡萄糖吡喃糖基-OMe(II)在水溶液中的优选构象和构象灵活性。两种三糖都具有邻位取代模式,其中长程(非顺序)相互作用可能起重要作用。600K下的LD模拟表明,全顺式构象占主导,不过其他构象也很明显。298K下的NOE数据以及MD和LD模拟均表明,三糖I在溶液中是单一的全顺式构象体。鉴于先前的研究显示β-D-葡萄糖吡喃糖基-(1→2)-β-D-葡萄糖吡喃糖基-(1→3)-α-D-葡萄糖吡喃糖基-OMe中存在反式构象体的证据,该结果提供了一个例子,说明将一个残基的异头构型从β变为α如何能使寡糖更刚性。通过实验和全顺式构象体模拟获得的环间距离存在差异,这表明II在β-(1→4)-连接处以反式ψ构象存在。对测量和计算的平移扩散常数以及(13)C T(1)弛豫时间进行联合分析,得出每种三糖的序参数为0.9。这意味着构象之间的任何相互转化都明显慢于翻滚。分别为I和II计算的各向异性约为1.6和1.3,这与观察到的相对平坦的T(1)谱一致,因为翻滚不在运动窄化区域。

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