Zelinski Björn, Müller Nina, Kierfeld Jan
Physics Department, TU Dortmund University, 44221 Dortmund, Germany.
Phys Rev E Stat Nonlin Soft Matter Phys. 2012 Oct;86(4 Pt 1):041918. doi: 10.1103/PhysRevE.86.041918. Epub 2012 Oct 31.
We investigate the microtubule polymerization dynamics with catastrophe and rescue events for three different confinement scenarios, which mimic typical cellular environments: (i) The microtubule is confined by rigid and fixed walls, (ii) it grows under constant force, and (iii) it grows against an elastic obstacle with a linearly increasing force. We use realistic catastrophe models and analyze the microtubule dynamics, the resulting microtubule length distributions, and force generation by stochastic and mean field calculations; in addition, we perform stochastic simulations. Freely growing microtubules exhibit a phase of bounded growth with finite microtubule length and a phase of unbounded growth. The main results for the three confinement scenarios are as follows: (i) In confinement by fixed rigid walls, we find exponentially decreasing or increasing stationary microtubule length distributions instead of bounded or unbounded phases, respectively. We introduce a realistic model for wall-induced catastrophes and investigate the behavior of the average length as a function of microtubule growth parameters. (ii) Under a constant force, the boundary between bounded and unbounded growth is shifted to higher tubulin concentrations and rescue rates. The critical force f(c) for the transition from unbounded to bounded growth increases logarithmically with tubulin concentration and the rescue rate, and it is smaller than the stall force. (iii) For microtubule growth against an elastic obstacle, the microtubule length and polymerization force can be regulated by microtubule growth parameters. For zero rescue rate, we find that the average polymerization force depends logarithmically on the tubulin concentration and is always smaller than the stall force in the absence of catastrophes and rescues. For a nonzero rescue rate, we find a sharply peaked steady-state length distribution, which is tightly controlled by microtubule growth parameters. The corresponding average microtubule length self-organizes such that the average polymerization force equals the critical force f(c) for the transition from unbounded to bounded growth. We also investigate the force dynamics if growth parameters are perturbed in dilution experiments. Finally, we show the robustness of our results against changes of catastrophe models and load distribution factors.
我们针对三种模拟典型细胞环境的不同限制情形,研究了具有灾难性事件和拯救事件的微管聚合动力学:(i)微管由刚性固定壁限制;(ii)微管在恒定力作用下生长;(iii)微管顶着弹性障碍物生长,且力呈线性增加。我们使用实际的灾难性模型,通过随机计算和平均场计算来分析微管动力学、由此产生的微管长度分布以及力的产生;此外,我们还进行了随机模拟。自由生长的微管呈现出有限微管长度的有界生长阶段和无界生长阶段。三种限制情形的主要结果如下:(i)在由固定刚性壁限制的情况下,我们分别发现了指数递减或递增的稳态微管长度分布,而非有界或无界阶段。我们引入了一个关于壁诱导灾难性事件的实际模型,并研究了平均长度作为微管生长参数函数的行为。(ii)在恒定力作用下,有界生长和无界生长之间的边界向更高的微管蛋白浓度和拯救速率偏移。从无界生长转变为有界生长的临界力f(c)随微管蛋白浓度和拯救速率呈对数增加,且小于失速力。(iii)对于顶着弹性障碍物生长的微管,微管长度和聚合力可由微管生长参数调节。对于零拯救速率,我们发现平均聚合力随微管蛋白浓度呈对数变化,且在没有灾难性事件和拯救事件的情况下总是小于失速力。对于非零拯救速率,我们发现了一个尖锐峰值的稳态长度分布,该分布由微管生长参数严格控制。相应的平均微管长度会自组织,使得平均聚合力等于从无界生长转变为有界生长的临界力f(c)。我们还在稀释实验中研究了生长参数受到扰动时的力动力学。最后,我们展示了我们的结果对于灾难性模型和负载分布因子变化的稳健性。