School of Engineering and Science, Jacobs University Bremen, Bremen, Germany.
J Phys Chem B. 2012 May 3;116(17):5141-51. doi: 10.1021/jp211564x. Epub 2012 Mar 22.
In this paper, a theoretical study of 1,2-dimethoxyethane (DME) and 1,2-dimethoxypropane (DMP) at water/n-heptane and 1,2-dimyristoyl-sn-glycero-3-phospatidycholine (DMPC) lipid bilayer/water interfaces using the umbrella sampling method is reported. Recently proposed GROMOS96/OPLS compatible models for DME and DMP have been used for the simulation studies. The percolation free energy barrier of one DME and DMP molecule from water to n-heptane phase calculated using the umbrella sampling method turned out to be equal to ~18.5 kJ/mol and ~6 kJ/mol, respectively. In the case of the DMPC lipid bilayer, overall free energy barriers of ~20 kJ/mol and ∼12 kJ/mol were obtained for DME and DMP, respectively. The spontaneous diffusion of DME and DMP in the lipid bilayer has also been investigated using unconstrained molecular dynamics simulations at the water/DMPC interface and inside the lipid bilayer. As expected from the estimated percolation barriers, simulation results show that DME, contrary to DMP, spontaneously diffuse into the aqueous solution from the lipid interior. In addition, simulations with multiple DME or DMP molecules at the interface show spontaneous diffusion within 50 ns inside the DMPC layer only for DMP.
本文采用伞状采样法研究了水/正庚烷和 1,2-二肉豆蔻酰基-sn-甘油-3-磷酸胆碱(DMPC)脂质双层/水界面上的 1,2-二甲氧基乙烷(DME)和 1,2-二甲氧基丙烷(DMP)的理论。最近提出的 GROMOS96/OPLS 兼容模型用于模拟研究。用伞状采样法计算的一个 DME 和 DMP 分子从水相到正庚烷相的渗透自由能势垒分别约为 18.5 kJ/mol 和 6 kJ/mol。在 DMPC 脂质双层的情况下,对于 DME 和 DMP,分别得到了约 20 kJ/mol 和 12 kJ/mol 的总自由能势垒。还使用在水/DMPC 界面和脂质双层内的无约束分子动力学模拟研究了 DME 和 DMP 在脂质双层中的自发扩散。根据估计的渗透势垒,模拟结果表明,与 DMP 相反,DME 从脂质内部自发扩散到水溶液中。此外,在界面处有多个 DME 或 DMP 分子的模拟中,仅对于 DMP,在 50 ns 内就可以在 DMPC 层内自发扩散。