Dembo M
Theoretical Biology and Biophysics, Los Alamos National Laboratory, New Mexico 87545.
Biophys J. 1989 Jun;55(6):1053-80. doi: 10.1016/S0006-3495(89)82904-2.
Many models of the cytoskeletal motility of Amoeba proteus can be formulated in terms of the theory of reactive interpenetrating flow (Dembo and Harlow, 1986). We have devised numerical methodology for testing such models against the phenomenon of steady axisymmetric fountain flow. The simplest workable scheme revealed by such tests (the minimal model) is the main preoccupation of this study. All parameters of the minimal model are determined from available data. Using these parameters the model quantitatively accounts for the self assembly of the cytoskeleton of A. proteus: for the formation and detailed morphology of the endoplasmic channel, the ectoplasmic tube, the uropod, the plasma gel sheet, and the hyaline cap. The model accounts for the kinematics of the cytoskeleton: the detailed velocity field of the forward flow of the endoplasm, the contraction of the ectoplasmic tube, and the inversion of the flow in the fountain zone. The model also gives a satisfactory account of measurements of pressure gradients, measurements of heat dissipation, and measurements of the output of useful work by amoeba. Finally, the model suggests a very promising (but still hypothetical) continuum formulation of the free boundary problem of amoeboid motion. by balancing normal forces on the plasma membrane as closely as possible, the minimal model is able to predict the turgor pressure and surface tension of A. proteus. Several dynamical factors are crucial to the success of the minimal model and are likely to be general features of cytoskeletal mechanics and control in amoeboid cells. These are: a constitutive law for the viscosity of the contractile network that includes an automatic process of gelation as the network density gets large; a very vigorous cycle of network polymerization and depolymerization (in the case of A. proteus, the time constant for this reaction is approximately 12 s); control of network contractility by a diffusible factor (probably calcium ion); and control of the adhesive interaction between the cytoskeleton and the inner surface of the plasma membrane.
许多变形虫细胞骨架运动的模型可以根据反应性互穿流理论来构建(Dembo和Harlow,1986年)。我们已经设计了数值方法,用于根据稳定轴对称喷泉流现象来测试此类模型。此类测试揭示的最简单可行方案(最小模型)是本研究的主要关注点。最小模型的所有参数均根据现有数据确定。利用这些参数,该模型定量地解释了变形虫细胞骨架的自组装:内质通道、外质管、尾足、质膜凝胶片和透明帽的形成及详细形态。该模型解释了细胞骨架的运动学:内质向前流动的详细速度场、外质管的收缩以及喷泉区流动的反转。该模型还令人满意地解释了压力梯度测量、热耗散测量以及变形虫有用功输出的测量结果。最后,该模型提出了一个非常有前景(但仍然是假设性的)关于变形虫运动自由边界问题的连续体公式。通过尽可能紧密地平衡质膜上的法向力,最小模型能够预测变形虫的膨压和表面张力。几个动力学因素对最小模型的成功至关重要,并且可能是变形虫细胞中细胞骨架力学和控制的普遍特征。这些因素包括:收缩网络粘度的本构定律,其中包括随着网络密度增大而自动发生的凝胶化过程;网络聚合和解聚的非常活跃的循环(就变形虫而言,此反应的时间常数约为12秒);通过可扩散因子(可能是钙离子)控制网络收缩性;以及控制细胞骨架与质膜内表面之间的粘附相互作用。