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本文引用的文献

1
Internal and environmental effects on folding and dimerization of the Alzheimer's β amyloid peptide.阿尔茨海默病β淀粉样肽折叠与二聚化的内在及环境影响
Mol Simul. 2011 May 1;37(6). doi: 10.1080/08927022.2011.551879.
2
Transmembrane structures for Alzheimer's Aβ(1-42) oligomers.跨膜结构对阿尔茨海默病 Aβ(1-42)寡聚物的影响。
J Am Chem Soc. 2010 Sep 29;132(38):13300-12. doi: 10.1021/ja103725c.
3
Probing the strand orientation and registry alignment in the propagation of amyloid fibrils.探测淀粉样纤维传播中的链取向和序列排列。
Biochemistry. 2010 Jun 29;49(25):5290-8. doi: 10.1021/bi100137y.
4
Thermodynamic perspective on the dock-lock growth mechanism of amyloid fibrils.从热力学角度看淀粉样纤维的对接锁定生长机制。
J Phys Chem B. 2009 Oct 29;113(43):14421-30. doi: 10.1021/jp9050098.
5
In silico study of full-length amyloid beta 1-42 tri- and penta-oligomers in solution.全长淀粉样β 1-42 三聚体和五聚体在溶液中的计算研究。
J Phys Chem B. 2009 Aug 27;113(34):11710-9. doi: 10.1021/jp901057w.
6
Dynamics of locking of peptides onto growing amyloid fibrils.肽段锁定到生长中的淀粉样纤维上的动力学。
Proc Natl Acad Sci U S A. 2009 Jul 21;106(29):11948-53. doi: 10.1073/pnas.0902473106. Epub 2009 Jul 6.
7
Structures and thermodynamics of Alzheimer's amyloid-beta Abeta(16-35) monomer and dimer by replica exchange molecular dynamics simulations: implication for full-length Abeta fibrillation.通过副本交换分子动力学模拟研究阿尔茨海默病淀粉样β蛋白Aβ(16 - 35)单体和二聚体的结构与热力学:对全长Aβ纤维化的启示
J Phys Chem B. 2009 May 28;113(21):7668-75. doi: 10.1021/jp900425e.
8
Replica exchange simulations of the thermodynamics of Abeta fibril growth.β-淀粉样蛋白纤维生长热力学的复制交换模拟
Biophys J. 2009 Jan;96(2):442-52. doi: 10.1016/j.bpj.2008.10.008.
9
The Alzheimer beta-amyloid (Abeta(1-39)) dimer in an implicit solvent.处于隐式溶剂中的阿尔茨海默病β-淀粉样蛋白(Abeta(1-39))二聚体
J Chem Phys. 2008 Nov 21;129(19):195102. doi: 10.1063/1.3021062.
10
Amyloid beta-protein monomer folding: free-energy surfaces reveal alloform-specific differences.淀粉样β蛋白单体折叠:自由能表面揭示了异构体特异性差异。
J Mol Biol. 2008 Dec 12;384(2):450-64. doi: 10.1016/j.jmb.2008.09.039. Epub 2008 Sep 24.

阿尔茨海默病 Aβ42 肽原纤维生长热力学的 replica 交换分子动力学。

Replica exchange molecular dynamics of the thermodynamics of fibril growth of Alzheimer's Aβ42 peptide.

机构信息

Department of Physics, Michigan Technological University, Houghton, Michigan 49931, USA.

出版信息

J Chem Phys. 2011 Aug 14;135(6):065101. doi: 10.1063/1.3617250.

DOI:10.1063/1.3617250
PMID:21842950
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3166336/
Abstract

The growth of amyloid fibrils is studied by replica exchange molecular dynamics in an implicit solvent. Our data indicate that extremely long simulation times (at least a few hundred ns) are necessary to study the thermodynamics of fibril elongation in detail. However some aspects of the aggregation process are already accessible on the time scales available in the present study. A peak in the specific heat indicates a docking temperature of T(dock) ≈ 320 K. Irreversible locking requires lower temperatures with the locking temperature estimated as T(lock) ≈ 280 K. In our simulation the fibril grows from both sides with the C-terminal of the incoming monomer attaching to the C-terminal of the peptides in the fibril forming a β-sheet on the fibril edge. Our simulation indicates that the C-terminal is crucial for aggregation.

摘要

在隐溶剂中通过复制交换分子动力学研究淀粉样纤维的生长。我们的数据表明,要详细研究纤维延伸的热力学,需要进行极长的模拟时间(至少几百纳秒)。然而,在本研究中可用的时间尺度上,已经可以研究聚合过程的某些方面。比热中的峰值表明对接温度 T(dock) ≈ 320 K。不可逆锁定需要较低的温度,锁定温度估计为 T(lock) ≈ 280 K。在我们的模拟中,纤维从两侧生长,进入的单体的 C 末端附着在纤维中的肽的 C 末端上,在纤维边缘形成 β-片层。我们的模拟表明,C 末端对于聚集至关重要。