Santo K P, Sebastian K L
Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore, India.
Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Dec;80(6 Pt 1):061801. doi: 10.1103/PhysRevE.80.061801. Epub 2009 Dec 10.
The dynamics of loop formation by linear polymer chains has been a topic of several theoretical and experimental studies. Formation of loops and their opening are key processes in many important biological processes. Loop formation in flexible chains has been extensively studied by many groups. However, in the more realistic case of semiflexible polymers, not much results are available. In a recent study [K. P. Santo and K. L. Sebastian, Phys. Rev. E 73, 031923 (2006)], we investigated opening dynamics of semiflexible loops in the short chain limit and presented results for opening rates as a function of the length of the chain. We presented an approximate model for a semiflexible polymer in the rod limit based on a semiclassical expansion of the bending energy of the chain. The model provided an easy way to describe the dynamics. In this paper, using this model, we investigate the reverse process, i.e., the loop formation dynamics of a semiflexible polymer chain by describing the process as a diffusion-controlled reaction. We make use of the "closure approximation" of Wilemski and Fixman [G. Wilemski and M. Fixman, J. Chem. Phys. 60, 878 (1974)], in which a sink function is used to represent the reaction. We perform a detailed multidimensional analysis of the problem and calculate closing times for a semiflexible chain. We show that for short chains, the loop formation time tau decreases with the contour length of the polymer. But for longer chains, it increases with length obeying a power law and so it has a minimum at an intermediate length. In terms of dimensionless variables, the closing time is found to be given by tau approximately Ln exp(const/L), where n=4.5-6. The minimum loop formation time occurs at a length Lm of about 2.2-2.4. These are, indeed, the results that are physically expected, but a multidimensional analysis leading to these results does not seem to exist in the literature so far.
线性聚合物链形成环的动力学一直是多个理论和实验研究的主题。环的形成及其打开是许多重要生物过程中的关键过程。柔性链中环的形成已被许多研究小组广泛研究。然而,在半柔性聚合物这种更实际的情况下,可用的结果并不多。在最近的一项研究中[K. P. 桑托和K. L. 塞巴斯蒂安,《物理评论E》73, 031923 (2006)],我们研究了短链极限下半柔性环的打开动力学,并给出了打开速率作为链长函数的结果。我们基于链弯曲能的半经典展开,提出了一个棒状极限下半柔性聚合物的近似模型。该模型提供了一种描述动力学的简便方法。在本文中,使用这个模型,我们研究相反的过程,即通过将半柔性聚合物链的环形成过程描述为扩散控制反应来研究其动力学。我们利用了维勒姆斯基和菲克斯曼的“封闭近似”[G. 维勒姆斯基和M. 菲克斯曼,《化学物理杂志》60, 878 (1974)],其中用一个汇函数来表示反应。我们对该问题进行了详细的多维分析,并计算了半柔性链的闭合时间。我们表明,对于短链,环形成时间τ随聚合物的轮廓长度减小。但对于较长的链,它随长度呈幂律增加,因此在中间长度处有一个最小值。用无量纲变量表示,发现闭合时间由τ≈Ln exp(const/L)给出,其中n = 4.5 - 6。最小环形成时间出现在长度Lm约为2.2 - 2.4处。这些确实是符合物理预期的结果,但迄今为止文献中似乎不存在导致这些结果的多维分析。