Commissariat à l'Energie Atomique, DSV/iBiTEC-S/SB2SM/LBMS & CNRS URA 2096, Centre d'Etudes, Saclay, F-91191 Gif-sur-Yvette Cedex, France.
J Phys Chem B. 2011 Jan 27;115(3):487-99. doi: 10.1021/jp109545v. Epub 2010 Dec 30.
This paper deals with the development and validation of new potential parameter sets, based on the CHARMM36 and GLYCAM06 force fields, to simulate micelles of the two anomeric forms (α and β) of N-dodecyl-β-maltoside (C(12)G(2)), a surfactant widely used in the extraction and purification of membrane proteins. In this context, properties such as size, shape, internal structure, and hydration of the C(12)G(2) anomer micelles were thoroughly investigated by molecular dynamics simulations and the results compared with experiments. Additional simulations were also performed with the older CHARMM22 force field for carbohydrates (Kuttel, M.; et al. J. Comput. Chem. 2002, 23, 1236-1243). We find that our CHARMM and GLYCAM parameter sets yield similar results in the case of properties related to the micelle structure but differ for other properties such as the headgroup conformation or the micelle hydration. In agreement with experiments, our results show that for all model potentials the β-C(12)G(2) micelles have a more pronounced ellipsoidal shape than those containing α anomers. The computed radius of gyration is 20.2 and 25.4 Å for the α- and β-anomer micelles, respectively. Finally, we show that depending on the potential the water translational diffusion of the interfacial water is 7-11.5 times slower than that of bulk water due to the entrapment of the water in the micelle crevices. This retardation is independent of the headgroup in α- or β-anomers.
本文致力于开发和验证新的潜在参数集,这些参数集基于 CHARMM36 和 GLYCAM06 力场,以模拟两种糖苷异构体(α 和β)的 N-十二烷基-β-麦芽糖苷(C(12)G(2))胶束。C(12)G(2)是一种广泛用于膜蛋白提取和纯化的表面活性剂。在这种情况下,通过分子动力学模拟彻底研究了 C(12)G(2)糖苷异构体胶束的大小、形状、内部结构和水合性质,并将结果与实验进行了比较。还使用较旧的 CHARMM22 碳水化合物力场(Kuttel,M.;等人,J. Comput. Chem.,2002,23,1236-1243)进行了额外的模拟。我们发现,在与胶束结构相关的性质方面,我们的 CHARMM 和 GLYCAM 参数集产生相似的结果,但在其他性质(如头基构象或胶束水合)方面则有所不同。与实验结果一致,我们的结果表明,对于所有模型势能,β-C(12)G(2)胶束的椭球形形状比含有α异构体的胶束更为明显。α-和β-异构体胶束的转动半径分别为 20.2 和 25.4 Å。最后,我们表明,根据势能的不同,界面水的平移扩散速度比体相水慢 7-11.5 倍,这是由于水被困在胶束的缝隙中。这种延迟与α或β-异构体中的头基无关。