May S, Harries D, Ben-Shaul A
Institut für Biochemie und Biophysik, Friedrich-Schiller-Universität Jena, Philosophenweg 12, 07743 Jena, Germany.
Biophys J. 2000 Oct;79(4):1747-60. doi: 10.1016/S0006-3495(00)76427-7.
The adsorption free energy of charged proteins on mixed membranes, containing varying amounts of (oppositely) charged lipids, is calculated based on a mean-field free energy expression that accounts explicitly for the ability of the lipids to demix locally, and for lateral interactions between the adsorbed proteins. Minimization of this free energy functional yields the familiar nonlinear Poisson-Boltzmann equation and the boundary condition at the membrane surface that allows for lipid charge rearrangement. These two self-consistent equations are solved simultaneously. The proteins are modeled as uniformly charged spheres and the (bare) membrane as an ideal two-dimensional binary mixture of charged and neutral lipids. Substantial variations in the lipid charge density profiles are found when highly charged proteins adsorb on weakly charged membranes; the lipids, at a certain demixing entropy penalty, adjust their concentration in the vicinity of the adsorbed protein to achieve optimal charge matching. Lateral repulsive interactions between the adsorbed proteins affect the lipid modulation profile and, at high densities, result in substantial lowering of the binding energy. Adsorption isotherms demonstrating the importance of lipid mobility and protein-protein interactions are calculated using an adsorption equation with a coverage-dependent binding constant. Typically, at bulk-surface equilibrium (i.e., when the membrane surface is "saturated" by adsorbed proteins), the membrane charges are "overcompensated" by the protein charges, because only about half of the protein charges (those on the hemispheres facing the membrane) are involved in charge neutralization. Finally, it is argued that the formation of lipid-protein domains may be enhanced by electrostatic adsorption of proteins, but its origin (e.g., elastic deformations associated with lipid demixing) is not purely electrostatic.
基于平均场自由能表达式计算带电荷蛋白质在含有不同数量(相反)带电荷脂质的混合膜上的吸附自由能,该表达式明确考虑了脂质局部相分离的能力以及吸附蛋白质之间的横向相互作用。使该自由能泛函最小化可得到熟悉的非线性泊松 - 玻尔兹曼方程以及膜表面允许脂质电荷重排的边界条件。这两个自洽方程同时求解。蛋白质被建模为均匀带电球体,(裸)膜被建模为带电和中性脂质的理想二维二元混合物。当高电荷蛋白质吸附在低电荷膜上时,发现脂质电荷密度分布有显著变化;脂质在一定的相分离熵罚的情况下,调整其在吸附蛋白质附近的浓度以实现最佳电荷匹配。吸附蛋白质之间的横向排斥相互作用影响脂质调制分布,并且在高密度时导致结合能大幅降低。使用具有覆盖度依赖结合常数的吸附方程计算表明脂质流动性和蛋白质 - 蛋白质相互作用重要性的吸附等温线。通常,在本体 - 表面平衡时(即当膜表面被吸附蛋白质“饱和”时),膜电荷被蛋白质电荷“过度补偿”,因为只有大约一半的蛋白质电荷(那些面向膜的半球上的电荷)参与电荷中和。最后,有人认为蛋白质的静电吸附可能会增强脂质 - 蛋白质结构域的形成,但其起源(例如与脂质相分离相关的弹性变形)并非纯粹是静电的。