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. 2024 Aug 8;14(1):18384.
doi: 10.1038/s41598-024-69422-3.

On the generation of force required for actin-based motility

Affiliations

On the generation of force required for actin-based motility

Alberto Salvadori et al. Sci Rep. .

Abstract

The fundamental question of how forces are generated in a motile cell, a lamellipodium, and a comet tail is the subject of this note. It is now well established that cellular motility results from the polymerization of actin, the most abundant protein in eukaryotic cells, into an interconnected set of filaments. We portray this process in a continuum mechanics framework, claiming that polymerization promotes a mechanical swelling in a narrow zone around the nucleation loci, which ultimately results in cellular or bacterial motility. To this aim, a new paradigm in continuum multi-physics has been designed, departing from the well-known theory of Larché-Cahn chemo-transport-mechanics. In this note, we set up the theory of network growth and compare the outcomes of numerical simulations with experimental evidence.

Keywords: Actin-based motility; Chemo-transport-mechanics; Continuum mechanics; Finite elements; High performance computing.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Figure 1
Figure 1
A 3D picture of the molecular components required for actin-based motility of Listeria monocytogenes.
Figure 2
Figure 2
Schematic representation of volume increment and protrusion upon the structural arrangement of monomers after polymerization of the dense actin filament network in lamellipodia (brown). The sparser actin network in the lamella is represented in purple. Scale bar, 1 μm. Inspired by.
Figure 3
Figure 3
Transient evolution of cF in time for different values of Ωf and kf, at cG0=2.42 moles m-3.
Figure 4
Figure 4
Simulation of the actin comet tail (colored) in Listeria monocytogenes (gray). (a) Mises stress; (b) actin concentration evolution in time at point A. In the simulations, the influence lengthscale of the signal is taken as =1.00μm.
Figure 5
Figure 5
(a) Transient evolution of cF in time, for ΩF=0.25 m3 moles-1 , kf=0.05 s-1, and cG0=2.42 moles m-3; (b) Evolution of the network velocity in time, for ΩF=0.25 m3 moles-1 , kf=0.05 s-1, and cG0=2.42 moles m-3. After an initial rapid development, the velocity is in agreement with the data, highlighted by the shaded strip. Data reported in correspond to the violet band (85±68nm/min).

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