ArticleNew journal of physics2014
Load sharing in the growth of bundled biopolymers.
Article in New journal of physics, 2014. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 7 papers.
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Who cites it
7 citing papers in PubMed.
- Energy-based modelling of single actin filament polymerization using bond graphs.Journal of the Royal Society, Interface · 2025Article
- Force-velocity relation and load-sharing in the linear polymerization ratchet revisited: the effects of barrier diffusion.The European physical journal. E, Soft matter · 2022Article
- Pulling-force generation by ensembles of polymerizing actin filaments.Physical biology · 2019Article
- Actin filaments pushing against a barrier: Comparison between two force generation mechanisms.The European physical journal. E, Soft matter · 2019Article
- Building a dendritic actin filament network branch by branch: models of filament orientation pattern and force generation in lamellipodia.Biophysical reviews · 2018Review
- Polymerisation force of a rigid filament bundle: diffusive interaction leads to sublinear force-number scaling.Scientific reports · 2018Article
- Steric Effects Induce Geometric Remodeling of Actin Bundles in Filopodia.Biophysical journal · 2016Article
Corrections and comments
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Authors and funding
2 authors.
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Abstract
To elucidate the nature of load sharing in the growth of multiple biopolymers, we perform stochastic simulations of the growth of biopolymer bundles against obstacles under a broad range of conditions and varying assumptions. The obstacle motion due to thermal fluctuations is treated explicitly. We assume the "Perfect Brownian Ratchet" (PBR) model, in which the polymerization rate equals the free-filament rate as soon as the filament-obstacle distance exceeds the monomer size. Accurate closed-form formulas are obtained for the case of a rapidly moving obstacle. We find the following: (1) load sharing is usually sub-perfect in the sense that polymerization is slower than for a single filament carrying the same average force; (2) the sub-perfect behavior becomes significant at a total force proportional to the logarithm or the square root of the number of filaments, depending on the alignment of the filaments; (3) for the special case of slow barrier diffusion and low opposing force, an enhanced obstacle velocity for an increasing number of filaments is possible; (4) the obstacle velocity is very sensitive to the alignment of the filaments in the bundle, with a staggered alignment being an order of magnitude faster than an unstaggered one at forces of only 0.5 pN per filament for 20 filaments; (5) for large numbers of filaments, the power is maximized at a force well below 1 pN per filament; (6) for intermediate values of the obstacle diffusion coefficient, the shape of the force velocity relation is very similar to that for rapid obstacle diffusion.
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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.