Mazur J, Jernigan R L
PRI/Dyncorp., Frederick Cancer Research Facility, Maryland 21702-1201.
Biopolymers. 1991 Nov;31(13):1615-29. doi: 10.1002/bip.360311316.
Detailed studies of structures of biological macromolecules, even in simplified models, involve many costly and time-consuming calculations. Any thorough methods require sampling of an extremely large conformation and momentum space. Calculations of electrostatic interactions, which depend on many physical factors, such as the details of solvent, solvent accessibility in macromolecules, and molecular polarizability, are always developed in a compromise between more rigorous, detailed models and the need for immediate application to complicated biological systems. In this paper, a middle ground is taken between the more exact theoretical models and the simplest constant values for the dielectric constant. The effects of solvent, counterions, and molecular polarizability are incorporated through a set of adjustable parameters that should be determined from experimental conditions. Several previous forms for the dielectric function are compared with the new ones. The present methods use Langevin functions to span the region of dielectric constant between bulk solvent and cavity values. Application of such dielectric models to double-helical DNA is important because base-stacking preferences were previously demonstrated [A. Sarai, J. Mazur, R. Nussinov, and R. L. Jernigan (1988) Biochemistry, vol. 27, pp. 8498-8502] to be sensitive to the electrostatic formulation. Here we find that poly(dG).poly(dC) can be A form for high screening and B form for low screening. By contrast, poly(dA).poly(dT) can only take the B form. Base stacking is more sensitive to the form of the dielectric function than are the sugar-phosphate backbone conformations. Also in B form, the backbone conformations are not so affected by the base types as in A form.
对生物大分子结构进行详细研究,即便采用简化模型,也涉及诸多成本高昂且耗时的计算。任何完备的方法都需要对极其庞大的构象和动量空间进行采样。静电相互作用的计算取决于许多物理因素,比如溶剂细节、大分子中溶剂可及性以及分子极化率,这类计算总是在更严谨、详细的模型与即刻应用于复杂生物系统的需求之间进行权衡。在本文中,我们在更精确的理论模型与最简单的介电常数常数值之间采取了折中的方法。通过一组应根据实验条件确定的可调参数纳入了溶剂、抗衡离子和分子极化率的影响。将几种先前的介电函数形式与新形式进行了比较。目前的方法使用朗之万函数来涵盖本体溶剂和空腔值之间的介电常数区域。将此类介电模型应用于双螺旋DNA很重要,因为先前已证明碱基堆积偏好 [A. 萨赖、J. 马祖尔、R. 努西诺夫和R. L. 杰尔尼根(1988年)《生物化学》,第27卷,第8498 - 8502页] 对静电公式很敏感。在此我们发现,聚(dG)·聚(dC)在高屏蔽时可为A构象,低屏蔽时可为B构象。相比之下,聚(dA)·聚(dT)只能呈B构象。碱基堆积对介电函数形式的敏感性高于糖 - 磷酸主链构象。同样在B构象中,主链构象不像在A构象中那样受碱基类型的影响那么大。