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超螺旋DNA的扩散控制链内反应:布朗动力学模拟

Diffusion-controlled intrachain reactions of supercoiled DNA: Brownian Dynamics simulations.

作者信息

Klenin K V, Langowski J

机构信息

Division of Biophysics of Macromolecules, German Cancer Research Center, D-69120, Heidelberg, Germany.

出版信息

Biophys J. 2001 Jan;80(1):69-74. doi: 10.1016/S0006-3495(01)75995-4.

Abstract

The Brownian Dynamics technique was used to model a diffusion-controlled intramolecular reaction of supercoiled DNA (2500 basepairs) in 0.1 M sodium chloride solution. The distance between the reactive groups along the DNA contour was 470 basepairs. The reaction radius was varied from 6 to 20 nm. The results are presented in terms of the probability distribution P(F)(t) of the first collision time. The general form of the function P(F)(t) could be correctly predicted by a simple analytical model of one-dimensional diffusion of the superhelix ends along the DNA contour. The distribution P(F)(t) is essentially non-exponential: within a large initial time interval, it scales as P(F)(t) approximately t(-1/2), which is typical for one-dimensional diffusion. However, the mean time of the first collision is inversely proportional to the reaction radius, as in three dimensions. A visual inspection of the simulated conformations showed that a considerable part of the collisions is caused by the bending of the superhelix axis in the regions of the end loops, where the axis is most flexible. This fact explains why the distribution P(F)(t) combines the features of one- and three-dimensional diffusion. The simulations were repeated for a DNA chain with a permanent bend of 100 degrees in the middle position between the reactive groups along the DNA contour. The permanent bend changes dramatically the form of the distribution P(F)(t) and reduces the mean time of the first collision by approximately one order of magnitude.

摘要

采用布朗动力学技术对超螺旋DNA(2500个碱基对)在0.1M氯化钠溶液中的扩散控制分子内反应进行建模。沿着DNA轮廓的反应基团之间的距离为470个碱基对。反应半径在6到20纳米之间变化。结果以首次碰撞时间的概率分布P(F)(t)呈现。通过超螺旋末端沿DNA轮廓的一维扩散的简单分析模型,可以正确预测函数P(F)(t)的一般形式。分布P(F)(t)本质上是非指数型的:在较大的初始时间间隔内,它的尺度为P(F)(t)约为t^(-1/2),这是一维扩散的典型特征。然而,首次碰撞的平均时间与反应半径成反比,这与三维情况相同。对模拟构象的直观检查表明,相当一部分碰撞是由超螺旋轴在末端环区域的弯曲引起的,在该区域轴最灵活。这一事实解释了为什么分布P(F)(t)兼具一维和三维扩散的特征。对于在沿着DNA轮廓的反应基团之间的中间位置有100度永久弯曲的DNA链重复进行了模拟。永久弯曲极大地改变了分布P(F)(t)的形式,并使首次碰撞的平均时间减少了大约一个数量级。

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