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从深度马尔可夫状态模型看一个无规卷曲蛋白的结合折叠途径。

Folding-upon-binding pathways of an intrinsically disordered protein from a deep Markov state model.

机构信息

Department of Chemistry, Dartmouth College, Hanover, NH 03755.

出版信息

Proc Natl Acad Sci U S A. 2024 Feb 6;121(6):e2313360121. doi: 10.1073/pnas.2313360121. Epub 2024 Jan 31.

DOI:10.1073/pnas.2313360121
PMID:38294935
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10861926/
Abstract

A central challenge in the study of intrinsically disordered proteins is the characterization of the mechanisms by which they bind their physiological interaction partners. Here, we utilize a deep learning-based Markov state modeling approach to characterize the folding-upon-binding pathways observed in a long timescale molecular dynamics simulation of a disordered region of the measles virus nucleoprotein N reversibly binding the X domain of the measles virus phosphoprotein complex. We find that folding-upon-binding predominantly occurs via two distinct encounter complexes that are differentiated by the binding orientation, helical content, and conformational heterogeneity of N. We observe that folding-upon-binding predominantly proceeds through a multi-step induced fit mechanism with several intermediates and do not find evidence for the existence of canonical conformational selection pathways. We observe four kinetically separated native-like bound states that interconvert on timescales of eighty to five hundred nanoseconds. These bound states share a core set of native intermolecular contacts and stable N helices and are differentiated by a sequential formation of native and non-native contacts and additional helical turns. Our analyses provide an atomic resolution structural description of intermediate states in a folding-upon-binding pathway and elucidate the nature of the kinetic barriers between metastable states in a dynamic and heterogenous, or "fuzzy", protein complex.

摘要

在研究无规卷曲蛋白质时,一个核心挑战是要阐明其与生理相互作用伴侣结合的机制。在这里,我们利用基于深度学习的马氏态模型方法,对麻疹病毒核蛋白 N 的无规区域与麻疹病毒磷酸蛋白复合物的 X 结构域可逆结合的长时程分子动力学模拟中观察到的折叠结合途径进行了特征描述。我们发现,折叠结合主要通过两种不同的结合前复合物发生,这两种复合物的区别在于 N 的结合取向、螺旋含量和构象异质性。我们观察到,折叠结合主要通过一个多步诱导契合机制进行,其中有几个中间产物,而且没有证据表明存在经典的构象选择途径。我们观察到四个动力学分离的类似天然的结合态,它们在八十到五百纳秒的时间尺度上相互转换。这些结合态共享一组核心的天然分子间接触和稳定的 N 螺旋,通过天然和非天然接触以及额外的螺旋转弯的顺序形成而有所区别。我们的分析提供了一个在折叠结合途径中中间状态的原子分辨率结构描述,并阐明了在动态和异质的、或“模糊”的蛋白质复合物中,亚稳态之间的动力学障碍的性质。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/c41dc6a97f9e/pnas.2313360121fig06.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/b26635c348c6/pnas.2313360121fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/b86064ac8deb/pnas.2313360121fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/bbc78254bc02/pnas.2313360121fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/d97c584c7250/pnas.2313360121fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/00a82d20a181/pnas.2313360121fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/c41dc6a97f9e/pnas.2313360121fig06.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/b26635c348c6/pnas.2313360121fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/b86064ac8deb/pnas.2313360121fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/bbc78254bc02/pnas.2313360121fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/d97c584c7250/pnas.2313360121fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/00a82d20a181/pnas.2313360121fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8b5d/10861926/c41dc6a97f9e/pnas.2313360121fig06.jpg

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