2015
DOI: 10.1209/0295-5075/110/48005
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Activity-driven fluctuations in living cells

Abstract: We propose a model for the dynamics of a probe embedded in a living cell, where both thermal fluctuations and nonequilibrium activity coexist. The model is based on a confining harmonic potential describing the elastic cytoskeletal matrix, which undergoes random active hops as a result of the nonequilibrium rearrangements within the cell. We describe the probe's statistics and we bring forth quantities affected by the nonequilibrium activity. We find an excellent agreement between the predictions of our model … Show more

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Cited by 123 publications
(163 citation statements)
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References 34 publications
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“…Reduced equations for random motion of both kinds of p-1 particles are derived. As we find, the derived equation for deformation tracers coincides with the previously proposed phenomenological model [9]. On the other hand, relative random motion of flow tracers with respect to the elastic component is described by a Langevin equation with non-thermal metabolic noise.…”
supporting
confidence: 85%
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“…Reduced equations for random motion of both kinds of p-1 particles are derived. As we find, the derived equation for deformation tracers coincides with the previously proposed phenomenological model [9]. On the other hand, relative random motion of flow tracers with respect to the elastic component is described by a Langevin equation with non-thermal metabolic noise.…”
supporting
confidence: 85%
“…The present analysis is however done entirely within the original description [10] in order to demonstrate what should be expected in its framework. Remarkably, we could then reproduce the phenomenological model [9] that shows good agreement with the experimental data for eukaryotic cells (see also the related publication [19]). Extensions and generalizations of our results to other models of gels can be performed, and this will be the task of additional work.…”
Section: P-2 Localization and Diffusion Of Tracer Particles In Viscoesupporting
confidence: 52%
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“…In soft-matter systems, examples include beads diffusing on lipid tubes (6), in actin and agarose networks (6)(7)(8)(9)(10), in concentrated colloidal suspensions (11,12), and in suspension with eukaryotic swimmers (13). For particles inside living cells, examples include RNA-protein particles and protein aggregates in Escherichia coli (14,15) and Saccharomyces cerevisiae (16) and submicron colloidal tracers in the cytoplasm of human cell lines (17,18). We suspect that there are many more examples to be found in biological systems, but studies involving single-particle tracking experiments in biological systems frequently do not report displacement distributions.…”
Section: Introductionmentioning
confidence: 99%
“…Caging model.-We propose a model for the vesicle dynamics and the effect of the surrounding fluctuating actin mesh that takes the observed power law behavior of G * into account. The model has itself been previously introduced in [30], but it is generalized here to encompass strong memory effects [31]. The underlying physical picture is that the vesicle is caged in the cytoskeleton [ Fig.…”
mentioning
confidence: 99%