Wang Ke, Yu Yang-Xin, Gao Guang-Hua, Luo Guang-Sheng
Department of Chemical Engineering, Tsinghua University, Beijing, 100084, People's Republic of China.
J Chem Phys. 2005 Dec 15;123(23):234904. doi: 10.1063/1.2137710.
A density-functional approach and canonical Monte Carlo simulations are presented for describing the ionic microscopic structure around the DNA molecule immersed in mixed-size counterion solutions. In the density-functional approach, the hard-sphere contribution to the Helmholtz energy functional is obtained from the modified fundamental measure theory [Y.-X. Yu and J. Z. Wu, J. Chem. Phys. 117, 10156 (2002)], and the electrostatic contribution is evaluated through a quadratic functional Taylor expansion. The new theory is suitable to the systems containing ions of arbitrary sizes and valences. In the established canonical Monte Carlo simulation, an iterative self-consistent method is used to evaluate the long-range energy, and another iterative algorithm is adopted to obtain desired bulk ionic concentrations. The ion distributions from the density-functional theory (DFT) are in good agreement with those from the corresponding Monte Carlo (MC) simulations. It is found that the ratio of the bulk concentrations of two species of counterions (cations) makes significant contribution to the ion distributions in the vicinity of DNA. Comparisons with the electrostatic potential profiles from the MC simulations show that the accuracy of the DFT becomes low when a small divalent cation exists. Both the DFT and MC simulation results illustrate that the electrostatic potential at the surface of DNA increases as the anion diameter or the total cation concentration is increased and decreases as the diameter of one cation species is increased. The calculation of electrostatic potential using real ion diameters shows that the accuracy of DFT predictions for divalent ions is also acceptable.
本文提出了一种密度泛函方法和正则蒙特卡罗模拟,用于描述浸没在混合尺寸抗衡离子溶液中的DNA分子周围的离子微观结构。在密度泛函方法中,亥姆霍兹能量泛函的硬球贡献是根据修正的基本度量理论[Y.-X. Yu和J. Z. Wu,《化学物理杂志》117, 10156 (2002)]获得的,静电贡献则通过二次泛函泰勒展开进行评估。该新理论适用于包含任意尺寸和价态离子的系统。在已建立的正则蒙特卡罗模拟中,采用迭代自洽方法来评估长程能量,并采用另一种迭代算法来获得所需的本体离子浓度。密度泛函理论(DFT)得到的离子分布与相应的蒙特卡罗(MC)模拟结果吻合良好。研究发现,两种抗衡离子(阳离子)的本体浓度之比对DNA附近的离子分布有显著贡献。与MC模拟得到的静电势分布进行比较表明,当存在少量二价阳离子时,DFT的精度会降低。DFT和MC模拟结果均表明,DNA表面的静电势随着阴离子直径或总阳离子浓度的增加而增加,随着一种阳离子物种直径的增加而减小。使用实际离子直径计算静电势表明,DFT对二价离子预测的精度也是可以接受的。