不对称离子浓度下的膜蛋白模拟

Fatemeh Khalili-Araghi, B. Ziervogel, B. Roux, J. Gumbart
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引用次数: 0

摘要

重要的细胞过程,如细胞-细胞识别、信号转导和电信号的传输都是由膜蛋白控制的。膜蛋白作为细胞环境的看门人,允许离子、小分子或新生蛋白在特定的环境信号下通过,如跨膜电压、离子浓度的变化或配体的结合。膜蛋白的分子动力学模拟,在脂质双层环境中进行,通过代表溶剂、脂质和蛋白质的完整原子细节来模拟细胞环境。这些模拟采用三维的周期性边界条件,以避免与系统有限尺寸相关的伪影。在这些条件下,膜蛋白系统被膜两侧的离子溶液包围,这些离子溶液的性质不能独立改变。我们开发了一种计算方法,可以在周期性边界条件下模拟膜蛋白,同时独立控制两种离子溶液的性质。在这种方法中,在两个相邻的单元胞之间引入能量屏障,将两个离子溶液分开。势垒的高度影响势垒两侧离子的化学势,因此可以单独控制离子的性质。在模拟过程中,势垒的高度被动态调整,以达到每侧合适的离子浓度。该方法已在分子动力学程序NAMD的Tcl接口中实现。我们应用该方法模拟生理条件下电压门控钾通道Kv1.2,其中胞外溶液由10mM KCl和100mM NaCl溶液组成,胞内溶液离子浓度为100mM KCl和10mM NaCl。在模拟中,两边的离子浓度保持1:10和10:1的比例。在100mV的电压偏置下进行了模拟,首次模拟了生理条件下的钾通道。该方法还被用于模拟在膜电位作用下通过外膜孔孔OmpF的离子电流。在这里,我们能够准确地计算出在10倍的盐梯度(0.1细胞内至1M细胞外KCl)下的OmpF通道的逆转电位。我们的结果与实验离子电导测量结果一致,重现了离子渗透和compf通道选择性的关键特征。具体来说,在不对称离子溶液下获得的I-V图揭示了通道中的自然不对称性,这是由于在正电位下观察到的电导率增加以及compf孔固有的阳离子选择性造成的。因此,我们开发了一种方法,直接将离子电流的分子动力学模拟与离子通道中的电生理测量联系起来。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Membrane protein simulations under asymmetric ionic concentrations
Important cellular processes, such as cell-cell recognition, signal transduction, and transport of electrical signals are controlled by membrane proteins. Membrane proteins act as gatekeepers of the cellular environment by allowing passage of ions, small molecules, or nascent proteins under specific environmental signals such as transmembrane voltage, changes in ionic concentration, or binding of a ligand. Molecular dynamics simulations of membrane proteins, performed in a lipid bilayer environment, mimic the cellular environment by representing the solvent, lipids, and the protein in full atomistic detail. These simulations employ periodic boundary conditions in three dimensions to avoid artifacts associated with the finite size of the system. Under these conditions, the membrane protein system is surrounded by ionic solutions on either side of the membrane whose properties cannot be changed independently. We have developed a computational method that allows simulations of membrane proteins under periodic boundary condition while controlling the two ionic solutions properties independently. In this method, an energy barrier is introduced between the two adjacent unit cells and separates the two ionic solutions. The height of the barrier affects the chemical potential of the ions on each side of the barrier, and thus allows for individual control over ionic properties. During the course of the simulation, the height of the barrier is adjusted dynamically to reach the proper ionic concentration on each side. This method has been implemented in the Tcl interface of the molecular dynamics program NAMD. We have applied this method to simulate the voltage-gated potassium channel Kv1.2 under physiological conditions, in which the extracellular solution is made of 10mM KCl and 100mM of NaCl solution, while the intracellular solution has an ionic concentration of 100mM KCl and 10mM NaCl. The simulations maintain a 1:10 and 10:1 ratio between ionic concentrations on each side. The simulations are performed under a voltage bias of 100mV and provide the first simulation of potassium channels under the exact physiological condition. The method has also been applied to simulate ionic currents passing through OmpF, an outer membrane porin, under membrane potentials. Here we were able to accurately calculate the reversal potential of the OmpF channel in a tenfold salt gradient of 0.1 intracellular to 1M extracellular KCl. Our results agree with experimental ion conductance measurements and reproduce key features of ion permeation and selectivity of the OmpF channel. Specifically, the I-V plots obtained under asymmetric ionic solutions revealed the natural asymmetry in the channel caused by increased conductance rates observed at positive potentials, as well as the inherent cation-selectivity of the OmpF pore. Therefore, we have developed a method that directly relates molecular dynamics simulations of ionic currents to electrophysiological measurements in ion channels.
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