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在高浓度结合位点极限情况下聚合物囊泡之间粘着斑的形成动力学

Adhesion plaque formation dynamics between polymer vesicles in the limit of highly concentrated binding sites.

作者信息

Nam Jin, Santore Maria M

机构信息

Department of Polymer Science and Engineering, University of Massachusetts-Amherst, 120 Governors Drive, Amherst, MA 01003, USA.

出版信息

Langmuir. 2007 Jun 19;23(13):7216-24. doi: 10.1021/la700542t. Epub 2007 May 25.

Abstract

This work examines the process of adhesion plaque formation between pairs of copolymer vesicles presenting dense surface concentrations of avidin (NeutrAvidin) and biotin. Micropipet aspiration maintains constant membrane tension, as the low-tension vesicle membrane spreads over a second, more tensed vesicle. Spreading rates near 1 microm/s but as high as 7 microm/s (the adhesion plaque diameter) and contact angle growth rates of 2-14 deg/s are observed. The ultimate contact angles, in the range of 120-140 degrees, are independent of membrane tension and also exceed those previously reported. Adhesion plaque formation occurs in three phases: an initial step in which contact is established, typically lasting from a few seconds to a minute, an abrupt jump into contact in which both vesicles undergo substantial deformation, and a slower continued growth of the contact angle and area. Vesicle pairs are irreversibly bound at the plaque such that attempts to peel them apart cause membrane rupture at critical tensions as high as 4 mN/m, setting a lower bound on the interfacial strength. When the quantity tau(1 - cos theta) (with tau the membrane tension and theta the contact angle) is plotted as a function of time during plaque formation for different values of tau, the curves fail to collapse, indicating the chemical driving force for adhesion greatly exceeds the mechanical resisting tension.

摘要

本研究考察了在表面呈现高密度抗生物素蛋白(中性抗生物素蛋白)和生物素的共聚物囊泡对之间形成黏附斑的过程。微量移液管抽吸可维持恒定的膜张力,此时低张力的囊泡膜会铺展在第二个张力更大的囊泡上。观察到铺展速率接近1微米/秒,但高达7微米/秒(黏附斑直径),接触角生长速率为2 - 14度/秒。最终接触角在120 - 140度范围内,与膜张力无关,且也超过了先前报道的值。黏附斑的形成分为三个阶段:首先是建立接触的初始步骤,通常持续几秒到一分钟;接着是突然进入接触阶段,此时两个囊泡都会发生显著变形;最后是接触角和接触面积的缓慢持续增长阶段。囊泡对在黏附斑处不可逆地结合,以至于试图将它们分开时,在高达4毫牛/米的临界张力下会导致膜破裂,从而确定了界面强度的下限。当针对不同的膜张力值τ,将τ(1 - cosθ)(其中τ为膜张力,θ为接触角)作为黏附斑形成过程中时间的函数进行绘制时,曲线无法重合,这表明黏附的化学驱动力大大超过了机械抵抗张力。

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