posted on 2024-05-08, 19:48authored byJoseph M. Barakat, Kevin J. Modica, Le Lu, Stephanie Anujarerat, Kyu Hwan Choi, Sho C. Takatori
Surface-bound molecular motors can drive the collective
motion
of cytoskeletal filaments in the form of nematic bands and polar flocks
in reconstituted gliding assays. Although these “swarming transitions”
are an emergent property of active filament collisions, they can be
controlled and guided by tuning the surface chemistry or topography
of the substrate. To date, the impact of surface topography on collective
motion in active nematics is only partially understood, with most
experimental studies focusing on the escape of a single filament from
etched channels. Since the late 1990s, significant progress has been
made to utilize the nonequilibrium properties of active filaments
and create a range of functional nanodevices relevant to biosensing
and parallel computation; however, the complexity of these swarming
transitions presents a challenge when attempting to increase filament
surface concentrations. In this work, we etch shallow, linear trenches
into glass substrates to induce the formation of swarming nematic
bands and investigate the mechanisms by which surface topography regulates
the two-dimensional (2D) collective motion of driven filamentous actin
(F-actin). We demonstrate that nematic swarms only appear at intermediate
trench spacings and vanish if the trenches are made too narrow, wide,
or tortuous. To rationalize these results, we simulate the F-actin
as self-propelled, semiflexible chains subject to a soft, spatially
modulated potential that encodes the energetic cost of bending a filament
along the edge of a trench. In our model, we hypothesize that an individual
filament experiences a penalty when its projected end-to-end distance
is smaller than the trench spacing (“bending and turning”).
However, chains that span the channel width glide above the trenches
in a force- and torque-free manner (“crowd-surfing”).
Our simulations demonstrate that collections of filaments form nematic
bands only at intermediate trench spacings, consistent with our experimental
findings.