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Bilayer Membrane in Confined Geometry: Interlayer Slide and Steric Repulsion

机译:受限几何中的双层膜:层间滑动和空间   推斥

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摘要

We derived free energy functional of a bilayer lipid membrane from the firstprinciples of elasticity theory. The model explicitly includesposition-dependent mutual slide of monolayers and bending deformation. Our freeenergy functional of liquid-crystalline membrane allows for incompressibilityof the membrane and vanishing of the in-plane shear modulus and obeysreflectional and rotational symmetries of the flat bilayer. Interlayer slide atthe mid-plane of the membrane results in local difference of surface densitiesof the monolayers. The slide amplitude directly enters free energy via thestrain tensor. For small bending deformations the ratio between bending modulusand area compression coefficient, Kb/KA, is proportional to the square ofmonolayer thickness, h. Using the functional we performed self-consistentcalculation of steric potential acting on bilayer between parallel confiningwalls separated by distance 2d. We found that temperature-dependent curvatureat the minimum of confining potential is enhanced four times for a bilayer withslide as compared with a unit bilayer. We also calculate viscous modes ofbilayer membrane between confining walls. Pure bending of the membrane isinvestigated, which is decoupled from area dilation at small amplitudes. Threesources of viscous dissipation are considered: water and membrane viscositiesand interlayer drag. Dispersion has two branches. Confinement between the wallsmodifies the bending mode with respect to membrane in bulk solution.Simultaneously, inter-layer slipping mode, damped by viscous drag, remainsunchanged by confinement.
机译:我们从弹性原理的第一原理中得出了双层脂质膜的自由能功能。该模型明确包括单层的位置相关的相互滑动和弯曲变形。我们的液晶膜的自由能功能允许膜的不可压缩性以及平面双层的平面内剪切模量和服从反射和旋转对称性的消失。在膜中平面的层间滑动导致单层表面密度的局部差异。滑动幅度通过应变张量直接输入自由能。对于较小的弯曲变形,弯曲模量与面积压缩系数之间的比率Kb / KA与单层厚度的平方h成正比。使用该功能,我们对相距2d的平行约束墙之间的双层进行了空间位势的自洽计算。我们发现,与双层单元相比,双层滑动层在最小限度电势下的温度相关曲率提高了四倍。我们还计算了围壁之间双层膜的粘性模式。研究了膜的纯弯曲,该弯曲在小幅度上与面积膨胀分离。考虑了粘性耗散的三种来源:水和膜的粘度以及层间阻力。分散体有两个分支。壁之间的限制改变了在整体溶液中相对于膜的弯曲模式。同时,层间打滑模式在粘性阻力的作用下仍然保持不变。

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