Demaret J P, Guéron M
Laboratoire de Physique et Chimie Biomoléculaires, Institut Curie, Paris, France.
Biophys J. 1993 Oct;65(4):1700-13. doi: 10.1016/S0006-3495(93)81213-X.
We develop and test a Poisson-Boltzmann model of the electrostatics of the B-Z transition of DNA. Starting from the detailed geometries of the two forms, we compute at each radius the fractions of DNA matter, of volume forbidden (for nonpoint-like ions), and of volume accessible to the center of ions. These radial distributions are incorporated in a composite cylinder model; availability to ions (porosity) and the dielectric constant at each radial distance are then obtained. The phosphate charge is distributed with cylindrical symmetry on two layers at the appropriate radial distances. The porous sheath, between the axis and the charge distribution, provides much more room for ions in B-DNA than in Z-DNA. By using previously developed methods, the Poisson-Boltzmann problem of such cylinders is easily solved. The computational load is small, so that results can be obtained for a large set of salt concentrations and for a number of ionic radii. The variation of the electrostatic free energy difference with salt concentration compares favorably with the experimental value (it is half as large). There is also qualitative agreement with experiments on supercoiled DNA, including a maximum of the free energy difference at submolar salt concentrations. The results for this cylinder with porous sheath are in line with those of the earlier simple planar model and of a plain cylinder with sheath, which is also presented here. They are thus insensitive to details of the model. They support the proposition that the main electrostatic feature of the B-Z transition is the better immersion of the B-DNA phosphates into the solution. They also give confidence in the validity of the Poisson-Boltzmann approach, despite the large salt concentrations involved. Prior studies using an approach based on the potential of mean force are discussed.
我们开发并测试了一个关于DNA B-Z转变静电学的泊松-玻尔兹曼模型。从两种形式的详细几何结构出发,我们计算了每个半径处DNA物质的分数、(对于非点状离子)禁止体积的分数以及离子中心可及体积的分数。这些径向分布被纳入一个复合圆柱模型;然后得到离子的可及性(孔隙率)和每个径向距离处的介电常数。磷酸根电荷以圆柱对称的方式分布在两个适当径向距离的层上。轴与电荷分布之间的多孔鞘层为B-DNA中的离子提供了比Z-DNA中更多的空间。通过使用先前开发的方法,这种圆柱体系的泊松-玻尔兹曼问题很容易求解。计算量很小,因此可以得到大量盐浓度和多种离子半径的结果。静电自由能差随盐浓度的变化与实验值相比具有较好的一致性(它只有实验值的一半大)。与超螺旋DNA的实验也存在定性的一致性包括在亚摩尔盐浓度下自由能差的最大值出现。这个带有多孔鞘层的圆柱体系的结果与早期简单平面模型以及这里也给出的带鞘层普通圆柱体系的结果一致。因此它们对模型细节不敏感。它们支持了这样的观点,即B-Z转变的主要静电特征是B-DNA磷酸根更好地浸入溶液中。它们也让人相信泊松-玻尔兹曼方法的有效性,尽管涉及到较大的盐浓度。文中还讨论了先前使用基于平均力势方法的研究。