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首页> 外文期刊>The Journal of Chemical Physics >Probing the mechanisms of fibril formation using lattice models
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Probing the mechanisms of fibril formation using lattice models

机译:用晶格模型探究原纤维形成的机理

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Using exhaustive Monte Carlo simulations we study the kinetics and mechanism of fibril formation using lattice models as a function of temperature (T) and the number of chains (M). While these models are, at best, caricatures of peptides, we show that a number of generic features thought to govern fibril assembly are captured by the toy model. The monomer, which contains eight beads made from three letters (hydrophobic, polar, and charged), adopts a compact conformation in the native state. In both the single-layered protofilament (seen for M <= 10) and the two-layer fibril (M>10) structures, the monomers are arranged in an antiparallel fashion with the "strandlike" conformation that is perpendicular to the fibril axis. Partial unfolding of the folded monomer that populates an aggregation prone conformation (N-*) is required for ordered assembly. The contacts in the N-* conformation, which is one of the four structures in the first "excited" state of the monomer, are also present in the native conformation. The time scale for fibril formation is a minimum in the T-range when the conformation N-* is substantially populated. The kinetics of fibril assembly occurs in three distinct stages. In each stage there is a cascade of events that transforms the monomers and oligomers to ordered structures. In the first "burst" stage, highly mobile oligomers of varying sizes form. The conversion to the N-* conformation occurs within the oligomers during the second stage in which a vast number of interchain contacts are established. As time progresses, a dominant cluster emerges that contains a majority of the chains. In the final stage, the aggregation of N-* particles serve as a template onto which smaller oligomers or monomers can dock and undergo conversion to fibril structures. The overall time for growth in the latter stages is well described by the Lifshitz-Slyazov growth kinetics for crystallization from supersaturated solutions. The detailed analysis shows that elements of the three popular models, namely, nucleation and growth, templated assembly, and nucleated conformational conversion are present at various stages of fibril assembly.
机译:使用详尽的蒙特卡洛模拟,我们使用晶格模型研究原纤维形成的动力学和机理,该动力学和机理是温度(T)和链数(M)的函数。虽然这些模型充其量只是肽的讽刺漫画,但我们证明玩具模型捕获了许多认为可控制原纤维组装的通用特征。该单体包含由三个字母(疏水,极性和带电)组成的八个珠子,在原始状态下呈紧密构象。在单层原丝(见M <= 10)和两层原纤维(M> 10)结构中,单体以反平行方式排列,并具有垂直于原纤维轴的“链状”构象。对于有序组装,需要折叠的单体的部分展开以形成易于聚集的构象(N- *)。 N- *构象中的接触是天然的构象,它是单体处于第一个“激发”状态的四个结构之一。当构象N- *基本存在时,原纤维形成的时间尺度在T范围内是最小的。原纤维组装的动力学发生在三个不同的阶段。在每个阶段都有一系列事件将单体和低聚物转变为有序结构。在第一个“爆发”阶段,形成了各种大小的高度可移动的低聚物。在建立大量链间接触的第二阶段,低聚物内发生向N- *构象的转化。随着时间的流逝,出现了一个占主导地位的集群,其中包含了大部分链条。在最后阶段,N- *粒子的聚集体作为模板,较小的低聚物或单体可以停靠在其上,并转化为原纤维结构。从过饱和溶液中结晶的Lifshitz-Slyazov生长动力学很好地描述了后期生长的总时间。详细分析表明,在原纤维组装的各个阶段都存在三种流行模型的元素,即成核和生长,模板组装和有核构象转化。

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