Pack G R, Garrett G A, Wong L, Lamm G
Department of Biomedical Sciences, University of Illinois College of Medicine at Rockford 61107.
Biophys J. 1993 Oct;65(4):1363-70. doi: 10.1016/S0006-3495(93)81187-1.
The results of variable dielectric coefficient Poisson-Boltzmann calculations of the counter-ion concentration in the vicinity of an all-atom model of the B-form of DNA are presented with an emphasis on the importance of spatial variations in the dielectric properties of the solvent, particularly at the macro-ion-solvent interface. Calculations of the distribution of hard-sphere electrolyte ions of various dimensions are reported. The presence of a dielectric boundary significantly increases the magnitude of the electrostatic potential with a concomitant increase in the accumulation of small counter-ions in the groove regions of DNA. Because ions with radii greater than 2 A have restricted access to the minor groove, the effect there is less significant than it is within the major groove. Changes in the dielectric coefficient for the electrolyte solution, allowing variation from 10 to 25, 40, 60, and 78.5 within the first 7.4 A of the surface of DNA, substantially increases the calculated surface concentration of counter-ions of all sizes. A lower dielectric coefficient near the macro-ion surface also tends to increase the counter-ion density in regions where the electrostatic potential is more negative than -kT. Regardless of the choice of dielectric coefficient, the number of ions in regions where the electrostatic potential is less than -kT remains the same for 0.153 M added 1-1 monovalent electrolyte as for the case without added salt. The strong dependence of the calculated distribution of counter-ion density on the choice of dielectric coefficients representing the solvent continuum suggests that care must be taken to properly characterize the physical system when studying electrostatic properties using these methods.
本文展示了对B型DNA全原子模型附近抗衡离子浓度进行可变介电系数泊松-玻尔兹曼计算的结果,重点强调了溶剂介电性质空间变化的重要性,特别是在大离子-溶剂界面处。报告了各种尺寸的硬球电解质离子分布的计算结果。介电边界的存在显著增加了静电势的大小,同时伴随着DNA沟槽区域中小抗衡离子积累的增加。由于半径大于2 Å的离子进入小沟的机会有限,因此那里的效应不如大沟内显著。电解质溶液介电系数的变化,允许在DNA表面的前7.4 Å内从10变化到25、40、60和78.5,大大增加了所有尺寸抗衡离子的计算表面浓度。大离子表面附近较低的介电系数也倾向于增加静电势比-kT更负的区域中的抗衡离子密度。无论介电系数如何选择,对于添加0.153 M 1-1单价电解质的情况,静电势小于-kT的区域中的离子数量与未添加盐的情况相同。计算得到的抗衡离子密度分布对代表溶剂连续介质的介电系数选择的强烈依赖性表明,在使用这些方法研究静电性质时,必须谨慎地正确表征物理系统。