Department of Biophysics , Bose Institute , P-1/12 CIT Scheme VII (M) , Kolkata 700054 , India.
Radiation Biology Branch , National Institutes of Health , Bethesda , Maryland 20814 , United States.
J Chem Inf Model. 2018 Aug 27;58(8):1576-1586. doi: 10.1021/acs.jcim.8b00169. Epub 2018 Aug 10.
The formation of amyloid fibers has been implicated in a number of neurodegenerative diseases. The growth of amyloid fibers is strongly thermodynamically favorable, but kinetic traps exist where the incoming monomer binds in an incompatible conformation that blocks further elongation. Unfortunately, this process is difficult to follow experimentally at the atomic level. It is also too complex to simulate in full detail and to date has been explored either through coarse-grained simulations, which may miss many important interactions, or full atomic simulations, in which the incoming peptide is constrained to be near the ideal fiber geometry. Here we use an alternate approach starting from a docked complex in which the monomer is from an experimental NMR structure of one of the major conformations in the unbound ensemble, a largely unstructured peptide with the central hydrophobic region in a 3 helix. A 1000 ns full atomic simulation in explicit solvent shows the formation of a metastable intermediate by sequential, concerted movements of both the fiber and the monomer. A Markov state model shows that the unfolded monomer is trapped at the end of the fiber in a set of interconverting antiparallel β-hairpin conformations. The simulation here may serve as a model for the binding of other non-β-sheet conformations to amyloid fibers.
淀粉样纤维的形成与许多神经退行性疾病有关。淀粉样纤维的生长在热力学上是非常有利的,但存在着动力学陷阱,即进入的单体以不兼容的构象结合,从而阻止进一步延伸。不幸的是,这个过程在原子水平上很难通过实验来跟踪。它也太复杂了,无法完整详细地模拟,迄今为止,人们要么通过粗粒度模拟来探索,这种模拟可能会错过许多重要的相互作用,要么通过全原子模拟来探索,在这种模拟中,进入的肽被约束在接近理想纤维几何形状的位置。在这里,我们从对接复合物开始采用一种替代方法,其中单体来自未结合态中主要构象之一的实验 NMR 结构,这是一种具有中央疏水区的 3 螺旋的大部分无结构肽。在明确溶剂中进行的 1000ns 全原子模拟显示,纤维和单体的连续协同运动形成了一个亚稳态中间体。马科夫状态模型表明,无规卷曲的单体在纤维末端被捕获在一组相互转化的反平行β发夹构象中。这里的模拟可能是其他非β-折叠构象与淀粉样纤维结合的模型。