Ho Bosco K, Thomas Annick, Brasseur Robert
Centre de Biophysique Moléculaire Numérique (CBMN), B-5030 Gembloux, Belgium.
Protein Sci. 2003 Nov;12(11):2508-22. doi: 10.1110/ps.03235203.
What determines the shape of the allowed regions in the Ramachandran plot? Although Ramachandran explained these regions in terms of 1-4 hard-sphere repulsions, there are discrepancies with the data where, in particular, the alphaR, alphaL, and beta-strand regions are diagonal. The alphaR-region also varies along the alpha-helix where it is constrained at the center and the amino terminus but diffuse at the carboxyl terminus. By analyzing a high-resolution database of protein structures, we find that certain 1-4 hard-sphere repulsions in the standard steric map of Ramachandran do not affect the statistical distributions. By ignoring these steric clashes (NH(i+1) and O(i-1)C), we identify a revised set of steric clashes (CbetaO, O(i-1)N(i+1), CbetaN(i+1), O(i-1)Cbeta, and O(i-1)O) that produce a better match with the data. We also find that the strictly forbidden region in the Ramachandran plot is excluded by multiple steric clashes, whereas the outlier region is excluded by only one significant steric clash. However, steric clashes alone do not account for the diagonal regions. Using electrostatics to analyze the conformational dependence of specific interatomic interactions, we find that the diagonal shape of the alphaR and alphaL-regions also depends on the optimization of the NH(i+1) and O(i-1)C interactions, and the diagonal beta-strand region is due to the alignment of the CO and NH dipoles. Finally, we reproduce the variation of the Ramachandran plot along the alpha-helix in a simple model that uses only H-bonding constraints. This allows us to rationalize the difference between the amino terminus and the carboxyl terminus of the alpha-helix in terms of backbone entropy.
是什么决定了拉氏图中允许区域的形状?尽管拉马钱德兰用1-4位硬球排斥来解释这些区域,但与数据存在差异,特别是αR、αL和β链区域是对角线状的。αR区域在α螺旋上也有变化,它在中心和氨基末端受到限制,而在羧基末端则是弥散的。通过分析蛋白质结构的高分辨率数据库,我们发现拉马钱德兰标准空间图中的某些1-4位硬球排斥并不影响统计分布。通过忽略这些空间冲突(NH(i+1)和O(i-1)C),我们确定了一组修正的空间冲突(CβO、O(i-1)N(i+1)、CβN(i+1)、O(i-1)Cβ和O(i-1)O),它们与数据的匹配度更好。我们还发现,拉氏图中的严格禁止区域是由多个空间冲突排除的,而异常值区域仅由一个显著的空间冲突排除。然而,仅空间冲突并不能解释对角线区域。利用静电学分析特定原子间相互作用的构象依赖性,我们发现αR和αL区域的对角线形状还取决于NH(i+1)和O(i-1)C相互作用的优化,而对角线β链区域是由于CO和NH偶极的排列。最后,我们在一个仅使用氢键约束的简单模型中重现了拉氏图沿α螺旋的变化。这使我们能够根据主链熵来解释α螺旋氨基末端和羧基末端之间的差异。