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通过分子动力学和自由能模拟研究Raf的Ras结合结构域的构象。

Conformation of the Ras-binding domain of Raf studied by molecular dynamics and free energy simulations.

作者信息

Zeng J, Treutlein H R, Simonson T

机构信息

Laboratoire de Biologie structurale, Illkirch (C.U. de Strasbourg), France.

出版信息

Proteins. 1998 May 1;31(2):186-200. doi: 10.1002/(sici)1097-0134(19980501)31:2<186::aid-prot8>3.0.co;2-k.

DOI:10.1002/(sici)1097-0134(19980501)31:2<186::aid-prot8>3.0.co;2-k
PMID:9593192
Abstract

Recognition of Ras by its downstream target Raf is mediated by a Ras-recognition region in the Ras-binding domain (RBD) of Raf. Residues 78-89 in this region occupy two different conformations in the ensemble of NMR solution structures of the RBD: a fully alpha-helical one, and one where 87-90 form a type IV beta-turn. Molecular dynamics simulations of the RBD in solution were performed to explore the stability of these and other possible conformations of both the wild-type RBD and the R89K mutant, which does not bind Ras. The simulations sample a fully helical conformation for residues 78-89 similar to the NMR helical structures, a conformation where 85-89 form a 3(10)-helical turn, and a conformation where 87-90 form a type I beta-turn, whose free energies are all within 0.3 kcal/mol of each other. NOE patterns and H(alpha) chemical shifts from the simulations are in reasonable agreement with experiment. The NMR turn structure is calculated to be 3 kcal/mol higher than the three above conformations. In a simulation with the same implicit solvent model used in the NMR structure generation, the turn conformation relaxes into the fully helical conformation, illustrating possible structural artifacts introduced by the implicit solvent model. With the Raf R89K mutant, simulations sample a fully helical and a turn conformation, the turn being 0.9 kcal/mol more stable. Thus, the mutation affects the population of RBD conformations, and this is expected to affect Ras binding. For example, if the fully helical conformation of residues 78-89 is required for binding, its free energy increase in R89K will increase the binding free energy by about 0.6 kcal/mol.

摘要

Ras的下游靶点Raf对Ras的识别是由Raf的Ras结合结构域(RBD)中的一个Ras识别区域介导的。该区域中的78-89位残基在RBD的NMR溶液结构集合中占据两种不同的构象:一种是完全α螺旋构象,另一种是87-90位形成IV型β转角的构象。对溶液中的RBD进行了分子动力学模拟,以探索野生型RBD和不结合Ras的R89K突变体的这些构象以及其他可能构象的稳定性。模拟结果显示,78-89位残基呈现出与NMR螺旋结构相似的完全螺旋构象、85-89位形成3(10)-螺旋转角的构象以及87-90位形成I型β转角的构象,它们的自由能彼此相差均在0.3 kcal/mol以内。模拟得到的NOE模式和H(α)化学位移与实验结果合理吻合。计算得出NMR转角结构比上述三种构象的能量高3 kcal/mol。在使用与NMR结构生成中相同的隐式溶剂模型进行的模拟中,转角构象松弛为完全螺旋构象,这说明了隐式溶剂模型可能引入的结构假象。对于Raf R89K突变体,模拟结果显示出完全螺旋构象和转角构象,其中转角构象更稳定,其自由能比完全螺旋构象低0.9 kcal/mol。因此,该突变影响了RBD构象的分布,预计这会影响Ras的结合。例如,如果78-89位残基的完全螺旋构象是结合所必需的,那么在R89K中其自由能的增加将使结合自由能增加约0.6 kcal/mol。

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