Ishida T, Yoneda S, Doi M, Inoue M, Kitamura K
Osaka University of Pharmaceutical Sciences, Japan.
Biochem J. 1988 Oct 15;255(2):621-8.
To investigate the biologically active conformation of enkephalin, molecular-dynamics simulations were applied to [Met5]- and [D-Ala2,Met5]-enkephalins. The dynamic trajectory of monomeric extended [Met5]-enkephalin was analysed in terms of relative mobility between respective torsions of backbone chain. After 10 ps of the dynamics simulation, the conformational transition was converged into a stationary state among the beta-bend folded forms, where they are stabilized by several intramolecular hydrogen-bond formations. Similar conformational transition was also observed in the dynamics simulation of [D-Ala2,Met5]enkephalin, which is a more mu-receptor-specific peptide than [Met5]enkephalin. The geometrical correspondence between the monomeric enkephalin conformation in the stationary state and morphine molecule (a mu-specific rigid opiate) was surveyed by virtue of the triangular substructures generated by choosing three functional atoms in each molecule, and good resemblances were observed. On the other hand, the dynamics simulation of the antiparallel extended [Met5]enkephalin dimer showed a trajectory different from that of the monomeric one. Two intermolecular hydrogen bonds at Tyr1 (NH3+)...Met5(CO2-) end residues were held throughout the 100 ps simulation, the dimeric structure being consequently kept. The conformational transition of the backbone chains from the antiparallel extended form to the twisted one took place via an intermediate state. Many conformations revealed during the dynamics simulation showed that the relative orientations of each two Tyr1, Gly3, Phe4 and Met5 residues in the dimer are nearly related by a pseudo-C2-symmetry respectively, and both halves of the dimer structure could be further fitted to the monomeric folded enkephalin conformation. The monomeric and dimeric conformations of enkephalin at their stationary states are discussed in relation to the substrate-specificity for mu- and delta-opioid receptors.
为了研究脑啡肽的生物活性构象,对[Met5]-脑啡肽和[D-Ala2,Met5]-脑啡肽进行了分子动力学模拟。根据主链各自扭转之间的相对迁移率,分析了单体伸展型[Met5]-脑啡肽的动态轨迹。在动力学模拟10皮秒后,构象转变收敛到β-转角折叠形式的稳定状态,这些形式通过几个分子内氢键的形成而稳定。在[D-Ala2,Met5]脑啡肽的动力学模拟中也观察到了类似的构象转变,[D-Ala2,Met5]脑啡肽是一种比[Met5]-脑啡肽更具μ-受体特异性的肽。通过选择每个分子中的三个功能原子生成的三角形子结构,研究了稳定状态下单体脑啡肽构象与吗啡分子(一种μ-特异性刚性阿片类药物)之间的几何对应关系,并观察到了良好的相似性。另一方面,反平行伸展型[Met5]-脑啡肽二聚体的动力学模拟显示出与单体不同的轨迹。在整个100皮秒的模拟过程中,Tyr1(NH3+)...Met5(CO2-)末端残基处的两个分子间氢键得以保持,从而使二聚体结构得以维持。主链从反平行伸展形式到扭曲形式的构象转变通过一个中间状态发生。动力学模拟过程中揭示的许多构象表明,二聚体中每两个Tyr1、Gly3、Phe4和Met5残基的相对取向分别通过伪C2对称性几乎相关,并且二聚体结构的两半可以进一步拟合到单体折叠的脑啡肽构象。讨论了脑啡肽在其稳定状态下的单体和二聚体构象与μ-和δ-阿片受体的底物特异性之间的关系。