Phase transition of DNA knotting in spherical space

结(造纸) 抗弯刚度 刚度(电磁) 持续时间 蒙特卡罗方法 几何学 DNA 物理 弯曲半径 概率分布 相空间 单调函数 经典力学 数学 弯曲 材料科学 数学分析 量子力学 化学 分子 热力学 扭转 统计 复合材料 生物化学
作者
Xiaolin Nie,Caiyun Xiong,Xun Zhou,Yanhui Liu
出处
期刊:Journal of Physics: Condensed Matter [IOP Publishing]
卷期号:34 (38): 385101-385101 被引量:1
标识
DOI:10.1088/1361-648x/ac808f
摘要

Knots have been discovered in various biological systems, such as DNA. The knotting probability of DNA in free space depends non-monotonically on its bending rigidity and has a prominent peak. The current work aims to understand the underlying mechanism of the non-monotonic dependence of DNA knotting probability on bending rigidity. Monte Carlo simulations are performed on a closed DNA molecule confined in spherical space described by a worm-like chain model and a flexible kink model, respectively. The closed DNA's contour length and the spherical space radius both increase knotting probability, but also alter the unimodal dependence of knotting probability on bending rigidity. This is generalized using universal phase diagrams based on the two models. Under the flexible kink model, the total knotting probability of closed DNA is obviously increased at a relatively high excited energy. This supports the expectation that the entropy effect of knot size favours knot formation at a relatively low bending rigidity. In a given spherical space, the increasing contour length of closed DNA described by the worm-like chain model results in a visible shift in the knotting probability distribution. At the same time, the gyration radius of non-trivial closed DNA becomes comparable to that of trivial closed DNA, so that their ratio is not anti-correlated with average knot length. For closed DNA of various contour lengths, the relationship between average knot length and bending rigidity has a universal behaviour: the average knot length decreases to a local minimum at a bending rigidity of ∼5 and then gradually increases to a constant value. The existence of the local minimum is determined by the cut-off distance in repulsive Lennard-Jones potential. The bending rigidity corresponding to the beginning of the constant average knot length is consistent with that at the peak in the knotting distribution. At this point, the knot-size effect balances with the fragment free-energy effect and, at an even greater bending rigidity, knot length breathes around the average knot length value.
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