首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Comparison of the Extended Isotropic Periodic Sum and Particle Mesh Ewald Methods for Simulations of Lipid Bilayers and Monolayers
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Comparison of the Extended Isotropic Periodic Sum and Particle Mesh Ewald Methods for Simulations of Lipid Bilayers and Monolayers

机译:扩展的各向同性周期总和与粒子网格Ewald方法对脂质双层和单层模拟的比较

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摘要

3D-IPS/DFFT is an extension of the three-dimensional isotropic periodic sum (3D-IPS) for evaluation of electrostatic and Lennard- Jones interactions in heterogeneous systems; it utilizes adiscrete fast Fourier transform (DFFT) for efficient calculation of the IPS potential with a large local region radius. The method is demonstrated to be highly accurate for simple bulk fluids, liquid/liquid and liquid/vapor interfaces, and lipid bilayers and monolayers. Values for r_c (the cutoff distance for direct evaluation of pairs) and R_c (the local region radius) equal to 10 A and twice the longest edge of the periodic cell, respectively, provide excellent efficiency and accuracy. Dimyristoylphosphatidylcholine (DMPC) monolayers simulated with the CHARMM (Chemistry at HARvard Molecular Mechanics) C27r lipid parameter set and 3D-IPS/DFFT yield surface tensions approximately 8 dyn/cm higher than those simulated using particle mesh Ewald (PME), and with experiment. In contrast, surface tensions for DMPC bilayers are 16 dyn/cm/leaflet with both 3D-IPS/DFFT (r_c = 10 and 12 A) and PME (r_c = 12 A). This indicates that PME (r_c = 12 A) may be used for simulations of bilayers, but not monolayers, and that the large bilayer surface tension arising from C27r is incorrect.
机译:3D-IPS / DFFT是三维各向同性周期总和(3D-IPS)的扩展,用于评估异构系统中的静电和Lennard-Jones相互作用。它利用离散的快速傅立叶变换(DFFT)来有效地计算具有较大局部半径的IPS电位。事实证明该方法对于简单的大体积流体,液体/液体和液体/蒸气界面以及脂质双层和单层是高度准确的。 r_c(直接评估线对的截止距离)和R_c(局部区域半径)的值分别等于10 A和周期单元最长边缘的两倍,可以提供出色的效率和准确性。使用CHARMM(哈佛分子化学)的C27r脂质参数集和3D-IPS / DFFT模拟的二肉豆蔻酰磷脂酰胆碱(DMPC)单层比使用粒子网格Ewald(PME)模拟的和实验的表面张力高约8 dyn / cm。相反,具有3D-IPS / DFFT(r_c = 10和12 A)和PME(r_c = 12 A)的DMPC双层的表面张力为16 dyn / cm /叶。这表明PME(r_c = 12 A)可以用于双层的模拟,但不能用于单层的模拟,并且由C27r引起的较大的双层表面张力是不正确的。

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