Evans E, Berk D, Leung A, Mohandas N
Department of Pathology, University of British Columbia, Vancouver, Canada.
Biophys J. 1991 Apr;59(4):849-60. doi: 10.1016/S0006-3495(91)82297-4.
As detailed in a companion paper (Berk, D., and E. Evans. 1991. Biophys. J. 59:861-872), a method was developed to quantitate the strength of adhesion between agglutinin-bonded membranes without ambiguity due to mechanical compliance of the cell body. The experimental method and analysis were formulated around controlled assembly and detachment of a pair of macroscopically smooth red blood cell surfaces. The approach provides precise measurement of the membrane tension applied at the perimeter of an adhesive contact and the contact angle theta c between membrane surfaces which defines the mechanical leverage factor (1-cos theta c) important in the definition of the work to separate a unit area of contact. Here, the method was applied to adhesion and detachment of red cells bound together by different monoclonal antibodies to red cell membrane glycophorin and the snail-helix pomatia-lectin. For these tests, one of the two red cells was chemically prefixed in the form of a smooth sphere then equilibrated with the agglutinin before the adhesion-detachment procedure. The other cell was not exposed to the agglutinin until it was forced into contact with the rigid cell surface by mechanical impingement. Large regions of agglutinin bonding were produced by impingement but no spontaneous spreading was observed beyond the forced contact. Measurements of suction force to detach the deformable cell yielded consistent behavior for all of the agglutinins: i.e., the strength of adhesion increased progressively with reduction in contact diameter throughout detachment. This tension-contact diameter behavior was not altered over a ten-fold range of separation rates. In special cases, contacts separated smoothly after critical tensions were reached; these were the highest values attained for tension. Based on measurements reported in another paper (Evans et al. 1991. Biophys. J. 59:838-848) of the forces required to rupture molecular-point attachments, the density of cross-bridges was estimated with the assumption that the tension was proportional to the discrete rupture force x the number of attachments per unit length. These estimates showed that only a small fraction of agglutinin formed cross-bridges at initial assembly and increased progressively with separation. When critical tension levels were reached, it appeared that nearly all local agglutinin was involved as cross-bridges. Because one cell surface was chemically fixed, receptor accumulation was unlikely; thus, microscopic "roughness" and steric repulsion probably modulated formation of cross-bridges on initial contact. To counter the steric repulsion, adhesive contacts were exposed to solutions of a high molecular weight polymer to draw the surfaces together by osmotic dehydration of the adhesion gap. These stresses exceeded initial mechanical assembly stresses by up to three orders of magnitude. As expected, the strength of adhesion was greatly enhanced by the added impingement stress.
正如一篇配套论文(伯克,D.,和E. 埃文斯。1991年。《生物物理杂志》59:861 - 872)中所详述的,已开发出一种方法来定量凝集素结合膜之间的粘附强度,而不会因细胞体的机械顺应性而产生歧义。实验方法和分析是围绕一对宏观光滑的红细胞表面的受控组装和分离来制定的。该方法提供了对施加在粘附接触周边的膜张力以及膜表面之间的接触角θc的精确测量,接触角θc定义了在分离单位面积接触时起重要作用的机械杠杆因子(1 - cosθc)。在此,该方法应用于通过不同单克隆抗体与红细胞膜糖蛋白和蜗牛 - 螺旋豆凝集素结合在一起的红细胞的粘附和分离。对于这些测试,两个红细胞中的一个以光滑球体的形式进行化学固定,然后在粘附 - 分离程序之前用凝集素进行平衡。另一个细胞直到通过机械撞击被迫与刚性细胞表面接触时才接触凝集素。通过撞击产生了大面积的凝集素结合,但在强制接触之外未观察到自发铺展。对分离可变形细胞的吸力测量得出所有凝集素的一致行为:即,在整个分离过程中粘附强度随着接触直径的减小而逐渐增加。这种张力 - 接触直径行为在分离速率的十倍范围内没有改变。在特殊情况下,在达到临界张力后接触会平稳分离;这些是所达到的最高张力值。根据另一篇论文(埃文斯等人。1991年。《生物物理杂志》59:838 - 848)中报道的破坏分子 - 点附着所需的力的测量结果,在假设张力与离散破裂力×每单位长度的附着数成正比的情况下,估计了交联桥的密度。这些估计表明,在初始组装时只有一小部分凝集素形成交联桥,并且随着分离逐渐增加。当达到临界张力水平时,似乎几乎所有局部凝集素都作为交联桥参与其中。由于一个细胞表面是化学固定的,受体积累不太可能;因此,微观“粗糙度”和空间排斥可能在初始接触时调节交联桥的形成。为了对抗空间排斥,将粘附接触暴露于高分子量聚合物溶液中,通过粘附间隙的渗透脱水将表面拉在一起。这些应力比初始机械组装应力高出多达三个数量级。正如预期的那样,添加的撞击应力大大增强了粘附强度。