Theory and Bio-Systems, Max Planck Institute of Colloids and Interfaces, 14424 Potsdam, Germany.
Soft Matter. 2022 Aug 17;18(32):6066-6078. doi: 10.1039/d2sm00618a.
Much effort has been devoted to lipid bilayers and nanovesicles with a compositional asymmetry between the two leaflets of the bilayer membranes. Here, we address another fundamental asymmetry related to lipid densities and membrane tensions. To avoid membrane rupture, the osmotic conditions must be adjusted in such a way that the bilayer membranes are subject to a relatively low bilayer tension. However, even for vanishing bilayer tension, the individual leaflets can still experience significant leaflet tensions if one leaflet is stretched whereas the other leaflet is compressed. Such a stress asymmetry between the two leaflets can be directly controlled in molecular dynamics simulations by the initial assembly of the lipid bilayers. This stress asymmetry is varied here over a wide range to determine the stability and instability regimes of the asymmetric bilayers. The stability regime shrinks with decreasing size and increasing membrane curvature of the nanovesicle. In the instability regimes, the lipids undergo stress-induced flip-flops with a flip-flop rate that increases with increasing stress asymmetry. The onset of flip-flops can be characterized by a cumulative distribution function that is well-fitted by an exponential function for planar bilayers but has a sigmoidal shape for nanovesicles. In addition, the bilayer membranes form transient non-bilayer structures that relax back towards ordered bilayers with a reduced stress asymmetry. Our study reveals intrinsic limits for the possible magnitude of the transbilayer stress asymmetry and shows that the leaflet tensions represent key parameters for the flip-flop rates.
人们在具有双层膜两叶之间组成不对称性的脂质双层和纳米囊泡上付出了大量努力。在这里,我们讨论与脂质密度和膜张力有关的另一个基本不对称性。为了避免膜破裂,必须调整渗透条件,以使双层膜承受相对较低的双层张力。然而,即使双层张力为零,只要一个叶层被拉伸而另一个叶层被压缩,那么两个叶层之间仍然会经历显著的叶层张力。这种双层之间的应力不对称性可以通过脂质双层的初始组装在分子动力学模拟中直接控制。在这里,通过改变初始组装,可以在很宽的范围内改变这种应力不对称性,以确定不对称双层的稳定和不稳定区域。随着纳米囊泡尺寸的减小和膜曲率的增加,稳定区域缩小。在不稳定区域,脂质会发生应力诱导的翻转,翻转速率随应力不对称性的增加而增加。翻转的开始可以通过累积分布函数来表征,对于平面双层,该函数可以很好地拟合指数函数,但对于纳米囊泡,该函数具有类正弦函数的形状。此外,双层膜会形成短暂的非双层结构,这些结构会松弛回到具有降低的应力不对称性的有序双层。我们的研究揭示了跨双层应力不对称性的可能幅度的内在限制,并表明叶层张力是翻转速率的关键参数。