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Actin polymerization kinetics, cap structure, and fluctuations

机译:肌动蛋白聚合动力学,帽结构和波动

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Polymerization of actin proteins into dynamic structures is essential to eukaryotic cell life, motivating many in vitro experiments measuring polymerization kinetics of individual filaments. Here, we model these kinetics, accounting for all relevant steps revealed by experiment: polymerization, depolymerization, random ATP hydrolysis, and release of phosphate (Pi). We relate filament growth rates to the dynamics of ATP-actin and ADP-P-i-actin caps that develop at filament ends. At the critical concentration of the barbed end, c(crit), we find a short ATP cap and a long fluctuation-stabilized ADP-Pi cap. We show that growth rates and the critical concentration at the barbed end are intimately related to cap structure and dynamics. Fluctuations in filament lengths are described by the length diffusion coefficient, D. Recently Fujiwara et al. [Fujiwara, L, Takahashi, S., Takaduma, H., Funatsu, T. & Ishiwata, S. (2002) Nat. Cell Biol. 4, 666-673] and Kuhn and Pollard [Kuhn, J. & Pollard, T. D. (2005) Biophys. J. 88, 1387-1402] observed large length fluctuations slightly above cc,it, provoking speculation that growth may proceed by oligomeric rather than monomeric on-off events. For the single-monomer growth process, we find that D exhibits a pronounced peak below c(crit), due to filaments alternating between capped and uncapped states, a mild version of the dynamic instability of microtubules. Fluctuations just above c(crit) are enhanced but much smaller than those reported experimentally. Future measurements of D as a function of concentration can help identify the origin of the observed fluctuations.
机译:肌动蛋白蛋白质聚合成动态结构对于真核细胞生命是必不可少的,从而激发了许多体外实验来测量单个长丝的聚合动力学。在这里,我们对这些动力学建模,说明实验揭示的所有相关步骤:聚合,解聚,无规ATP水解和磷酸盐(Pi)的释放。我们将细丝生长速率与在细丝末端形成的ATP-肌动蛋白和ADP-P-i-肌动蛋白帽的动力学联系起来。在刺入端的临界浓度c(crit)下,我们发现ATP上限很短,而稳定ADP-Pi上限很长。我们表明,增长率和刺入端的临界浓度与瓶盖结构和动力学密切相关。长丝长度的波动由长度扩散系数D来描述。 [Fujiwara,L,Takahashi,S.,Takaduma,H.,Funatsu,T.&Ishiwata,S.(2002)Nat。细胞生物学。 4,666-673]和Kuhn and Pollard [Kuhn,J.&Pollard,T. D.(2005)Biophys。 [J. 88,1387-1402]观察到较大的长度波动,略高于cc,it,这引发了人们猜测生长可能是通过寡聚而不是单体的开关事件来进行的。对于单单体的生长过程,我们发现D在c(crit)以下显示一个明显的峰,这是由于细丝在封端和未封端状态之间交替变化,是微管动态不稳定性的温和形式。高于c(crit)的波动有所增强,但比实验报告的波动小得多。 D作为浓度函数的未来测量值可以帮助识别观察到的波动的根源。

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