Marzec C J, Day L A
Public Health Research Institute, New York, New York 10016.
Biophys J. 1993 Dec;65(6):2559-77. doi: 10.1016/S0006-3495(93)81313-4.
The capsids of the spherical viruses all show underlying icosahedral symmetry, yet they differ markedly in capsomere shape and in capsomere position and orientation. The capsid patterns presented by the capsomere shapes, positions, and orientations of three viruses (papilloma, SV40, and N beta V) have been generated dynamically through a bottom-up procedure which provides a basis for understanding the patterns. A capsomere shape is represented in two-dimensional cross-section by a mass or charge density on the surface of a sphere, given by an expansion in spherical harmonics, and referred to herein as a morphological unit (MU). A capsid pattern is represented by an icosahedrally symmetrical superposition of such densities, determined by the positions and orientations of its MUs on the spherical surface. The fitness of an arrangement of MUs is measured by an interaction integral through which all capsid elements interact with each other via an arbitrary function of distance. A capsid pattern is generated by allowing the correct number of approximately shaped MUs to move dynamically on the sphere, positioning themselves until an extremum of the fitness function is attained. The resulting patterns are largely independent of the details of both the capsomere representation and the interaction function; thus the patterns produced are generic. The simplest useful fitness function is sigma 2, the average square of the mass (or charge) density, a minimum of which corresponds to a "uniformly spaced" MU distribution; to good approximation, the electrostatic free energy of charged capsomeres, calculated from the linearized Poisson-Boltzmann equation, is proportional to sigma 2. With disks as MUs, the model generates the coordinated lattices familiar from the quasi-equivalence theory, indexed by triangulation numbers. Using fivefold MUs, the model generates the patterns observed at different radii within the T = 7 capsid of papilloma and at the surface of SV40; threefold MUs give the T = 4 pattern of Nudaurelia capensis beta virus. In all cases examined so far, the MU orientations are correctly found.
球形病毒的衣壳均呈现出潜在的二十面体对称性,但它们在衣壳粒形状、衣壳粒位置和方向上存在显著差异。通过自下而上的程序动态生成了三种病毒(乳头瘤病毒、SV40病毒和NβV病毒)的衣壳粒形状、位置和方向所呈现的衣壳模式,这为理解这些模式提供了基础。衣壳粒形状在二维横截面中由球体表面的质量或电荷密度表示,通过球谐展开给出,在此称为形态学单位(MU)。衣壳模式由这种密度的二十面体对称叠加表示,由其在球面上的MU的位置和方向决定。MU排列的适应性通过相互作用积分来衡量,通过该积分,所有衣壳元件通过距离的任意函数相互作用。通过允许正确数量的近似形状的MU在球面上动态移动,定位自身直到达到适应度函数的极值,从而生成衣壳模式。所得模式在很大程度上独立于衣壳粒表示和相互作用函数的细节;因此产生的模式是通用的。最简单有用的适应度函数是σ²,即质量(或电荷)密度的平均平方,其最小值对应于“均匀间隔”的MU分布;从线性化的泊松-玻尔兹曼方程计算的带电衣壳粒的静电自由能与σ²近似成比例。以圆盘作为MU,该模型生成了从准等价理论中熟知的协调晶格,由三角剖分数索引。使用五重MU,该模型生成了在乳头瘤病毒T = 7衣壳内不同半径处以及SV40表面观察到的模式;三重MU给出了卡普斯纳裸病毒的T = 4模式。在迄今为止检查的所有情况下,都正确找到了MU的方向。