Collective motion of dimers

Catherine J. Penington, Karolína Korvasová, Barry D. Hughes, and Kerry A. Landman
Phys. Rev. E 86, 051909 – Published 9 November 2012

Abstract

We consider a discrete agent-based model on a one-dimensional lattice and a two-dimensional square lattice, where each agent is a dimer occupying two sites. Agents move by vacating one occupied site in favor of a nearest-neighbor site and obey either a strict simple exclusion rule or a weaker constraint that permits partial overlaps between dimers. Using indicator variables and careful probability arguments, a discrete-time master equation for these processes is derived systematically within a mean-field approximation. In the continuum limit, nonlinear diffusion equations that describe the average agent occupancy of the dimer population are obtained. In addition, we show that multiple species of interacting subpopulations give rise to advection-diffusion equations. Averaged discrete simulation data compares very well with the solution to the continuum partial differential equation models. Since many cell types are elongated rather than circular, this work offers insight into population-level behavior of collective cellular motion.

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  • Received 19 June 2012

DOI:https://doi.org/10.1103/PhysRevE.86.051909

©2012 American Physical Society

Authors & Affiliations

Catherine J. Penington, Karolína Korvasová, Barry D. Hughes, and Kerry A. Landman*

  • Department of Mathematics and Statistics, University of Melbourne, Victoria 3010, Australia

  • *kerryl@unimelb.edu.au

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Issue

Vol. 86, Iss. 5 — November 2012

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