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β-发夹折叠中来自备选未折叠构象的微观事件。

Microscopic events in β-hairpin folding from alternative unfolded ensembles.

机构信息

Department of Chemistry, Cambridge University, Lensfield Road, Cambridge CB2 1EW, United Kingdom.

出版信息

Proc Natl Acad Sci U S A. 2011 Jul 5;108(27):11087-92. doi: 10.1073/pnas.1016685108. Epub 2011 Jun 20.

Abstract

We have performed the first unbiased folding simulations of the GB1 hairpin in explicit solvent, using hundreds of microsecond-long molecular dynamics simulations (total time: 0.7 ms). Our simulations are initiated from two sets of structures. Starting from an equilibrium unfolded state, we obtain single-exponential folding kinetics with rate coefficients in good agreement (T=350 K) or within an order of magnitude (T=300 K) of the experimental values. However, simulations initiated from unfolded configurations lacking secondary structure result in biexponential kinetics with an additional fast nanosecond kinetic mode. This mode can strongly bias the folding rate estimated from the mean first passage time, when the trials are much shorter than the folding time. We find that the mechanism of the hairpin folding is insensitive to the details of the initial unfolded ensemble and is initiated by correct formation of the turn of the hairpin, followed by the formation of the native hydrogen bonds and hydrophobic contacts, consistent with experimental -value analysis. Subsequent native interactions can be formed either from the turn or from the hairpin termini, helping to explain an apparent discrepancy in experimental results. From our simulations, we also obtain the transition path durations, a critical parameter for single molecule experiments aiming to resolve events along folding pathways. The lengths of transition paths span a wide range, from 50 ps to 140 ns, at 300 K.

摘要

我们在显式溶剂中对 GB1 发夹进行了首次无偏折叠模拟,使用了数百个微秒长的分子动力学模拟(总时间:0.7 毫秒)。我们的模拟是从两组结构开始的。从平衡展开状态开始,我们获得了单指数折叠动力学,其速率系数与实验值非常吻合(T=350 K)或在数量级内(T=300 K)。然而,从缺乏二级结构的展开构象开始的模拟导致双指数动力学,其中存在额外的快速纳秒动力学模式。当试验时间远短于折叠时间时,这种模式会强烈偏向于从平均首次通过时间估计的折叠速率。我们发现发夹折叠的机制对初始展开集合的细节不敏感,由发夹转弯的正确形成引发,随后是形成天然氢键和疏水接触,与实验值分析一致。随后的天然相互作用可以从转弯处或发夹末端形成,有助于解释实验结果中的明显差异。从我们的模拟中,我们还获得了过渡路径持续时间,这是旨在解析折叠途径中事件的单分子实验的关键参数。在 300 K 时,过渡路径的长度范围很宽,从 50 ps 到 140 ns。

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