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荷电涨落对柔性聚两性电解质形状的影响及其在天然无序蛋白质中的应用。

Charge fluctuation effects on the shape of flexible polyampholytes with applications to intrinsically disordered proteins.

机构信息

Department of Chemistry, University of Texas at Austin, Austin, Texas 78712, USA.

出版信息

J Chem Phys. 2018 Oct 28;149(16):163323. doi: 10.1063/1.5035428.

Abstract

Random polyampholytes (PAs) contain positively and negatively charged monomers that are distributed randomly along the polymer chain. The interaction between charges is assumed to be given by the Debye-Huckel potential. We show that the size of the PA is determined by an interplay between electrostatic interactions, giving rise to the polyelectrolyte effect due to net charge per monomer () and an effective attractive PA interaction due to charge fluctuations, . The interplay between these terms gives rise to non-monotonic dependence of the radius of gyration, , on the inverse Debye length, , when PA effects are important ( ). In the opposite limit, decreases monotonically with increasing . Simulations of PA chains, using a charged bead-spring model, further corroborate our theoretical predictions. The simulations unambiguously show that conformational heterogeneity manifests itself among sequences that have identical PA parameters. A clear implication is that the phases of PA sequences, and by inference intrinsically disordered proteins (IDPs), cannot be determined using only the bare PA parameters ( and ). The theory is used to calculate the changes in on , the number of residues for a set of IDPs. For a certain class of IDPs, with between 24 and 441, the size grows as ∼ , which agrees with data from small angle X-ray scattering experiments.

摘要

无规多聚物(PAs)含有沿聚合物链随机分布的正电荷和负电荷单体。电荷之间的相互作用假定由 Debye-Huckel 势能给出。我们表明,PA 的大小取决于静电相互作用的相互作用,由于每个单体的净电荷()而产生聚电解质效应,并且由于电荷波动而产生有效的吸引力 PA 相互作用。这些术语之间的相互作用导致当 PA 效应很重要时(),回转半径的非单调依赖性,,相对于逆 Debye 长度。在相反的极限下,随着的增加而单调减小。使用带电珠-弹簧模型对 PA 链的模拟进一步证实了我们的理论预测。模拟清楚地表明,具有相同 PA 参数的序列表现出构象异质性。一个明显的含义是,PA 序列的相,以及推断的固有无序蛋白质(IDPs),不能仅使用裸 PA 参数(和)来确定。该理论用于计算在,一组 IDPs 的残基数上的变化。对于具有 24 到 441 之间的特定 IDP 类,大小增长为 ∼,这与小角度 X 射线散射实验的数据一致。

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