Evans C W, Proctor J
J Cell Sci. 1978 Oct;33:17-36. doi: 10.1242/jcs.33.1.17.
We have obtained data on the frequency of aggregates of different size classes and on the maximum aggregate diameter of lymphoid cells subjected to aggregation in the laminar shear field of a Couette viscometer. Maximum aggregate diameter reached a plateau level during aggregation. This plateau is considered to be the result of a balance between the hydrodynamic shear forces tending to resist the formation of aggregates, and the adhesive forces of the aggregated cells tending to resist dissociation. Stepwise-increases in the shear rate produced aggregates of progressively smaller maximum diameter until the limiting (i.e. control equivalent) diameter was reached. Equations governing these stepwise changes in aggregate diameter were obtained by regression analysis, and an estimate of the force of dissociation (FD) was made from derived values of the critical shear rate. Thymocytes (FD=2.54 X 10(-6) N m-2/cell) were found to be more adhesive than lymphocytes (FD=2.05 X 10(-6) N m-2/cell), in agreement with current concepts. The observed data on aggregate frequency were seen to be of poor fit with a model of aggregation derived by collision analysis of the aggregation process. This led us to consider the possibility that all cells may not share the same probability of forming an adhesion. We thus derived further models of aggregation in which some fraction of the total cells was considered to have enhanced possibilities of a collision producing an adhesion. Of the models we considered, a 15% preferred fraction offered best agreement with the experimental observations. We therefore conclude that the populations of cells studied in this report are not 'homogenous' in that some cells are more adhesive than others. Alterations in the percentage of the preferred fraction of cells will lead to different aggregate-frequency indices. Such changes might be expected to occur during the initial stages of carcinoma development.
我们已获取了不同尺寸级别的聚集体频率数据,以及在库埃特粘度计层流剪切场中发生聚集的淋巴细胞的最大聚集体直径数据。在聚集过程中,最大聚集体直径达到了一个平稳水平。这个平稳状态被认为是由趋于阻止聚集体形成的流体动力剪切力与趋于阻止解离的聚集细胞的粘附力之间的平衡所导致的。剪切速率的逐步增加产生了最大直径逐渐变小的聚集体,直到达到极限(即对照等效)直径。通过回归分析得到了控制聚集体直径这些逐步变化的方程,并根据临界剪切速率的推导值对解离力(FD)进行了估计。胸腺细胞(FD = 2.54×10⁻⁶ N m⁻²/细胞)被发现比淋巴细胞(FD = 2.05×10⁻⁶ N m⁻²/细胞)更具粘附性,这与当前的概念一致。观察到的聚集体频率数据与通过对聚集过程进行碰撞分析得出的聚集模型拟合度较差。这使我们考虑到所有细胞可能不具有相同的形成粘附的概率。因此,我们推导了进一步的聚集模型,其中总细胞的一部分被认为具有更高的碰撞产生粘附的可能性。在我们考虑的模型中,15%的优先部分与实验观察结果最为吻合。因此,我们得出结论,本报告中研究的细胞群体并非“同质的”,因为一些细胞比其他细胞更具粘附性。优先部分细胞百分比的改变将导致不同的聚集频率指数。在癌症发展的初始阶段可能会出现这样的变化。