Kuzmin Peter I, Akimov Sergey A, Chizmadzhev Yuri A, Zimmerberg Joshua, Cohen Fredric S
Laboratory of Cellular and Molecular Biophysics, National Institute of Child Health and Human Development, National Institutes of Health, Bethesda, Maryland 20892, USA.
Biophys J. 2005 Feb;88(2):1120-33. doi: 10.1529/biophysj.104.048223. Epub 2004 Nov 12.
Membrane domains known as rafts are rich in cholesterol and sphingolipids, and are thought to be thicker than the surrounding membrane. If so, monolayers should elastically deform so as to avoid exposure of hydrophobic surfaces to water at the raft boundary. We calculated the energy of splay and tilt deformations necessary to avoid such hydrophobic exposure. The derived value of energy per unit length, the line tension gamma, depends on the elastic moduli of the raft and the surrounding membrane; it increases quadratically with the initial difference in thickness between the raft and surround; and it is reduced by differences, either positive or negative, in spontaneous curvature between the two. For zero spontaneous curvature, gamma is approximately 1 pN for a monolayer height mismatch of approximately 0.3 nm, in agreement with experimental measurement. Our model reveals conditions that could prevent rafts from forming, and a mechanism that can cause rafts to remain small. Prevention of raft formation is based on our finding that the calculated line tension is negative if the difference in spontaneous curvature for a raft and the surround is sufficiently large: rafts cannot form if gamma < 0 unless molecular interactions (ignored in the model) are strong enough to make the total line tension positive. Control of size is based on our finding that the height profile from raft to surround does not decrease monotonically, but rather exhibits a damped, oscillatory behavior. As an important consequence, the calculated energy of interaction between rafts also oscillates as it decreases with distance of separation, creating energy barriers between closely apposed rafts. The height of the primary barrier is a complex function of the spontaneous curvatures of the raft and the surround. This barrier can kinetically stabilize the rafts against merger. Our physical theory thus quantifies conditions that allow rafts to form, and further, defines the parameters that control raft merger.
被称为筏区的膜结构域富含胆固醇和鞘脂,并且被认为比周围的膜更厚。如果是这样,单分子层应该会发生弹性变形,以避免在筏区边界处疏水表面暴露于水中。我们计算了避免这种疏水暴露所需的张开和倾斜变形能量。推导出的每单位长度的能量值,即线张力γ,取决于筏区和周围膜的弹性模量;它随着筏区与周围区域初始厚度差异的平方而增加;并且它会因两者之间自发曲率的正负差异而减小。对于零自发曲率,当单分子层高度失配约为0.3纳米时,γ约为1皮牛,这与实验测量结果一致。我们的模型揭示了可能阻止筏区形成的条件,以及一种可导致筏区保持较小尺寸的机制。阻止筏区形成是基于我们的发现:如果筏区和周围区域的自发曲率差异足够大,计算出的线张力为负;如果γ < 0,除非分子间相互作用(模型中忽略)足够强以使总线张力为正,否则筏区无法形成。尺寸控制基于我们的发现:从筏区到周围区域的高度分布并非单调下降,而是呈现出一种衰减的振荡行为。一个重要的结果是,计算出的筏区之间的相互作用能量也会随着它们之间分离距离的减小而振荡,在紧密相邻的筏区之间形成能量障碍。主要障碍的高度是筏区和周围区域自发曲率的复杂函数。这种障碍可以从动力学上稳定筏区以防止合并。因此,我们的物理理论量化了允许筏区形成的条件,并且进一步定义了控制筏区合并的参数。