A single active ring model with velocity self-alignment

Cellular tissue behavior is a multiscale problem. At the cell level, out of equilibrium, biochemical reactions drive physical cell-cell interactions in a typical active matter process. Cell modeling computer simulations are a robust tool to explore countless possibilities and test hypotheses. Here,...

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Veröffentlicht in:Soft matter 2021-06, Vol.17 (24), p.5991-6
Hauptverfasser: Teixeira, Emanuel F, Fernandes, Heitor C. M, Brunnet, Leonardo G
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Sprache:eng
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Zusammenfassung:Cellular tissue behavior is a multiscale problem. At the cell level, out of equilibrium, biochemical reactions drive physical cell-cell interactions in a typical active matter process. Cell modeling computer simulations are a robust tool to explore countless possibilities and test hypotheses. Here, we introduce a two-dimensional, extended active matter model for biological cells. A ring of interconnected self-propelled particles represents the cell. Neighboring particles are subject to harmonic and bending potentials. Within a characteristic time, each particle's self-velocity tends to align with its scattering velocity after an interaction. Translational modes, rotational modes, and mixtures of these appear as collective states. Using analytical results derived from active Brownian particles, we identify effective characteristic time scales for ballistic and diffusive movements. Finite-size scale investigation shows that the ring diffusion increases linearly with its size when in collective movement. A study on the ring shape reveals that all collective states are present even when bending forces are weak. In that case, when in a translational mode, the collective velocity aligns with the largest ring's direction in a spontaneous polarization emergence. Active particles held together in a ring. Decreasing bending and noise intensities induces a change from a persistent random walk to an expontaneous collective motion polarized along the larger ring dimension, guiding the movement.
ISSN:1744-683X
1744-6848
DOI:10.1039/d1sm00080b