Symmetry and stability of orientationally ordered collective motions of self-propelled, semiflexible filaments

TL;DR

This study uses simulations to explore how active, semiflexible filaments self-organize into ordered states, revealing the roles of filament overlap, flexibility, and active forces in forming nematic or polar collective motions.

Contribution

It demonstrates that long-range order depends on filament overlap and flexibility, and identifies conditions under which nematic or polar states emerge as steady states.

Findings

Long-range order requires filament overlap in the absence of aligning torques.

Symmetry of order (nematic or polar) depends on filament overlap energy and flexibility.

Active polar order is the only steady state for systems with finite filament rigidity.

Abstract

Ordered, collective motions commonly arise spontaneously in systems of many interacting, active units, ranging from cellular tissues and bacterial colonies to self-propelled colloids and animal flocks. Active phases are especially rich when the active units are sufficiently anisotropic to produce liquid crystalline order and thus active nematic phenomena, with important biophysical examples provided by cytoskeletal filaments including microtubules and actin. Gliding assay experiments have provided a testbed to study the collective motions of these cytoskeletal filaments and unlocked diverse collective active phases, including states with long-range orientational order. However, it is not well-understood how such long-range order emerges from the interplay of passive and active aligning mechanisms. We use Brownian dynamics simulations to study the collective motions of semiflexible filaments that self-propel in quasi-two dimensions, in order to gain insights into the aligning mechanisms at work in these gliding assay systems. We find that, without aligning torques in the microscopic model, long-range orientational order can only be achieved when the filaments are able to overlap. The symmetry (nematic or polar) of the long-range order that first emerges is shown to depend on the energy cost of filament overlap and on filament flexibility. However, our model also predicts that a long-range-ordered active nematic state is merely transient, whereas long-range polar order is the only active dynamical steady state in systems with finite filament rigidity.