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大球体熵驱动插入圆柱形容器的动力学。

Dynamics of the entropic insertion of a large sphere into a cylindrical vessel.

作者信息

Hara Ryohei, Amano Ken-ichi, Kinoshita Masahiro, Yoshimori Akira

机构信息

Department of Physics, Kyushu University, Fukuoka 812-8581, Japan.

Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan.

出版信息

J Chem Phys. 2016 Mar 14;144(10):105103. doi: 10.1063/1.4943394.

Abstract

Insertion of a solute into a vessel comprising biopolymers is a fundamental function in a biological system. The entropy originating from the translational displacement of solvent particles plays an essential role in the insertion. Here we study the dynamics of entropic insertion of a large spherical solute into a cylindrical vessel. The solute and the vessel are immersed in small spheres forming the solvent. We develop a theoretical method formulated using the Fokker-Planck equation. The spatial distribution of solute-vessel entropic potential, which is calculated by the three-dimensional integral equation theory combined with rigid-body models, serves as input data. The key quantity analyzed is the density of the probability of finding the solute at any position at any time. It is found that the solute is inserted along the central axis of the vessel cavity and trapped at a position where the entropic potential takes a local minimum value. The solute keeps being trapped without touching the vessel inner surface. In a significantly long time τ, the solute transfers to the position in contact with the vessel bottom possessing the global potential minimum along the central axis. As the solute size increases, τ becomes remarkably longer. We also discuss the relevance of our result to the functional expression of a chaperonin/cochaperonin in the assistance of protein folding.

摘要

将溶质插入包含生物聚合物的容器中是生物系统中的一项基本功能。溶剂粒子平移位移产生的熵在插入过程中起着至关重要的作用。在此,我们研究了一个大的球形溶质向圆柱形容器中进行熵插入的动力学过程。溶质和容器浸没在构成溶剂的小球体中。我们开发了一种基于福克 - 普朗克方程的理论方法。通过三维积分方程理论结合刚体模型计算得到的溶质 - 容器熵势的空间分布用作输入数据。所分析的关键量是在任意时刻溶质处于任意位置的概率密度。结果发现,溶质沿着容器腔的中心轴插入,并被困在熵势取局部最小值的位置。溶质一直被困住,不接触容器内表面。在相当长的时间τ内,溶质转移到沿着中心轴与具有全局势最小值的容器底部接触的位置。随着溶质尺寸增大,τ变得显著更长。我们还讨论了我们的结果与伴侣蛋白/共伴侣蛋白在协助蛋白质折叠中的功能表达的相关性。

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