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蛋白质泛素的3纳秒分子动力学模拟及其与X射线晶体结构和溶液核磁共振结构的比较。

3 Nsec molecular dynamics simulation of the protein ubiquitin and comparison with X-ray crystal and solution NMR structures.

作者信息

Braatz J A, Paulsen M D, Ornstein R L

机构信息

Molecular Science Research Center, Pacific Northwest Laboratory, Richland, WA.

出版信息

J Biomol Struct Dyn. 1992 Apr;9(5):935-49. doi: 10.1080/07391102.1992.10507968.

Abstract

Mainly due to computational limitations, past protein molecular dynamics simulations have rarely been extended to 300 psec; we are not aware of any published results beyond 350 psec. The present work compares a 3000 psec simulation of the protein ubiquitin with the available x-ray crystallographic and solution NMR structures. Aside from experimental structure availability, ubiquitin was studied because of its relatively small size (76 amino acids) and lack of disulfide bridges. An implicit solvent model was used except for explicit treatment of waters of crystallization. We found that the simulated average structure retains most of the character of the starting x-ray crystal structure. In two highly surface accessible regions, the simulation was not in agreement with the x-ray structure. In addition, there are six backbone-backbone hydrogen bonds that are in conflict between the solution NMR and x-ray crystallographic structures; two are bonds that the NMR does not locate, and four are ones that the two methods disagree upon the donor. Concerning these six backbone-backbone hydrogen bonds, the present simulation agrees with the solution NMR structure in five out-of-the six cases, in that if a hydrogen bond is present in the x-ray structure and not in the NMR structure, the bond breaks within 700 psec. Of the two hydrogen bonds that are found in the NMR structure and not in the x-ray structure, one forms at 1400 psec and the other forms rarely. The present results suggest that relatively long molecular dynamics simulations, that use protein x-ray crystal coordinates for the starting structure and a computationally efficient solvent representation, may be used to gain an understanding of conformational and dynamic differences between the solid-crystal and dilute-solution states.

摘要

主要由于计算能力的限制,过去的蛋白质分子动力学模拟很少能扩展到300皮秒;我们不知道有任何超过350皮秒的已发表结果。本研究将蛋白质泛素的3000皮秒模拟与现有的X射线晶体学结构和溶液核磁共振结构进行了比较。除了实验结构的可获得性外,选择泛素进行研究是因为其相对较小的尺寸(76个氨基酸)且缺乏二硫键。除了对结晶水进行显式处理外,使用了隐式溶剂模型。我们发现模拟得到的平均结构保留了起始X射线晶体结构的大部分特征。在两个高度暴露于表面的区域,模拟结果与X射线结构不一致。此外,溶液核磁共振结构和X射线晶体学结构之间存在六个主链-主链氢键相互冲突;其中两个是核磁共振未定位到的键,另外四个是两种方法在供体上存在分歧的键。关于这六个主链-主链氢键,本模拟在六个案例中的五个与溶液核磁共振结构一致,即如果一个氢键存在于X射线结构中而不存在于核磁共振结构中,该键会在700皮秒内断裂。在核磁共振结构中发现而在X射线结构中未发现的两个氢键中,一个在1400皮秒形成,另一个很少形成。目前的结果表明,使用蛋白质X射线晶体坐标作为起始结构并采用计算效率高的溶剂表示法的相对较长的分子动力学模拟,可用于了解固态晶体状态和稀溶液状态之间的构象和动力学差异。

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