Evans E A
Biophys J. 1985 Jul;48(1):185-92. doi: 10.1016/S0006-3495(85)83771-1.
In general, membrane-membrane adhesion involves specific molecular binding and cross-bridging reactions. The ideal, classical view is that near equilibrium the forces required to separate adhesive contacts are essentially equal to those induced in the membrane when the contact is formed. In contrast to the classical view, experimental observations often show that negligible levels of tension are induced by the adhesive contact even though the tension required to separate the contact is large enough to rupture the membrane. The deviation in tension levels associated with contact formation and separation appears to be due to the sparse distribution of strong molecular cross-bridges. Here, the mechanics of membrane-membrane adhesion and separation is developed for the case of discrete, kinetically trapped cross-bridges. The solution is obtained by numerical computation of the membrane contour that minimizes the total free energy (membrane elastic energy of deformation plus cross-bridge energies) in the contact zone. This solution is matched with the analytical solution for membrane stresses and geometry derived for the adjacent, unbridged zone. The results yield specific values of the macroscopic tension applied to the membrane in the plane region away from the contact zone and the microscopic angle at the edge of the contact zone. Two disparate values of the macroscopic tension are found: (a) the minimum tension required to separate the adherent membranes; and (b) the maximum tension induced in the membranes when the contact is formed (i.e., the level of tension at which the contact will just begin to spread). The results show that the deviation between these two tensions can be very large and depends strongly on the surface density of cross-bridges. In addition, the results provide an estimate of the restraining forces that anchor receptors within the plane of the membrane.
一般来说,膜 - 膜粘附涉及特定的分子结合和交联反应。理想的经典观点是,在接近平衡时,分离粘附接触所需的力基本上等于形成接触时在膜中诱导的力。与经典观点相反,实验观察结果常常表明,即使分离接触所需的张力大到足以使膜破裂,粘附接触所诱导的张力水平也可以忽略不计。与接触形成和分离相关的张力水平偏差似乎是由于强分子交联桥的稀疏分布所致。在此,针对离散的、动力学捕获的交联桥情况,推导了膜 - 膜粘附和分离的力学原理。通过对膜轮廓进行数值计算来获得解决方案,该计算使接触区域内的总自由能(膜变形的弹性能加交联桥能量)最小化。此解决方案与为相邻的非桥接区域推导的膜应力和几何形状的解析解相匹配。结果给出了在远离接触区域的平面区域中施加到膜上的宏观张力的特定值以及接触区域边缘处的微观角度。发现了两个不同的宏观张力值:(a) 分离粘附膜所需的最小张力;(b) 形成接触时在膜中诱导的最大张力(即接触即将开始扩展时的张力水平)。结果表明,这两种张力之间的偏差可能非常大,并且强烈依赖于交联桥的表面密度。此外,结果还提供了对将受体锚定在膜平面内的约束力的估计。