Varma Sameer, Chiu See-Wing, Jakobsson Eric
Center for Biophysics and Computational Biology, National Center for Supercomputing Applications, Department of Biochemistry, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA.
Biophys J. 2006 Jan 1;90(1):112-23. doi: 10.1529/biophysj.105.059329. Epub 2005 Sep 23.
Several groups, including our own, have found molecular dynamics (MD) calculations to result in the size of the pore of an outer membrane bacterial porin, OmpF, to be reduced relative to its size in the x-ray crystal structure. At the narrowest portion of its pore, loop L3 was found to move toward the opposite face of the pore, resulting in decreasing the cross-section area by a factor of approximately 2. In an earlier work, we computed the protonation states of titratable residues for this system and obtained values different from those that had been used in previous MD simulations. Here, we show that MD simulations carried out with these recently computed protonation states accurately reproduce the cross-sectional area profile of the channel lumen in agreement with the x-ray structure. Our calculations include the investigation of the effect of assigning different protonation states to the one residue, D(127), whose protonation state could not be modeled in our earlier calculation. We found that both assumptions of charge states for D(127) reproduced the lumen size profile of the x-ray structure. We also found that the charged state of D(127) had a higher degree of hydration and it induced greater mobility of polar side chains in its vicinity, indicating that the apparent polarizability of the D(127) microenvironment is a function of the D(127) protonation state.
包括我们自己的团队在内,有几个研究小组发现,分子动力学(MD)计算得出的外膜细菌孔蛋白OmpF的孔径相对于其X射线晶体结构中的尺寸有所减小。在其孔的最窄部分,发现环L3向孔的相对面移动,导致横截面积减小了约2倍。在早期的一项工作中,我们计算了该系统中可滴定残基的质子化状态,并得到了与先前MD模拟中使用的值不同的结果。在这里,我们表明,用这些最近计算出的质子化状态进行的MD模拟准确地再现了与X射线结构一致的通道内腔的横截面积分布。我们的计算包括研究将不同质子化状态赋予一个残基D(127)的影响,在我们早期的计算中无法模拟其质子化状态。我们发现,D(127)的两种电荷状态假设都再现了X射线结构的内腔尺寸分布。我们还发现,D(127)的带电状态具有更高程度的水合作用,并且它在其附近诱导了极性侧链更大的流动性,这表明D(127)微环境的表观极化率是D(127)质子化状态的函数。