2021
DOI: 10.1073/pnas.2106038118
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Submersed micropatterned structures control active nematic flow, topology, and concentration

Abstract: Coupling between flows and material properties imbues rheological matter with its wide-ranging applicability, hence the excitement for harnessing the rheology of active fluids for which internal structure and continuous energy injection lead to spontaneous flows and complex, out-of-equilibrium dynamics. We propose and demonstrate a convenient, highly tunable method for controlling flow, topology, and composition within active films. Our approach establishes rheological coupling via the indirect presence of ful… Show more

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Cited by 46 publications
(45 citation statements)
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References 68 publications
(83 reference statements)
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“…Beyond substrate friction, recent work has studied the effects of a different type of external dissipation on active nematic turbulence [28,146]. Instead of on a solid substrate, active nematic microtubule films can be assembled at an oil-water interface.…”
Section: Interaction With An External Fluidmentioning
confidence: 99%
“…Beyond substrate friction, recent work has studied the effects of a different type of external dissipation on active nematic turbulence [28,146]. Instead of on a solid substrate, active nematic microtubule films can be assembled at an oil-water interface.…”
Section: Interaction With An External Fluidmentioning
confidence: 99%
“…Surface patterning can also be realized using a smectic oil, which can provide an anisotropic environment and render the turbulent-like, active nematic flows into more ordered flows ( 23 , 24 ). More recently, a submersed micropatterned surface also demonstrates the capability of control over defect dynamics and spontaneous flows in microtubule-based active nematic film ( 54 ). We anticipate that our concept of activity patterning could be combined with these different patterning techniques and may lead to unprecedented phenomena and new applications.…”
Section: Discussionmentioning
confidence: 99%
“…where we have defined the parameter z = 4(αR 2 0 γ )/(Kγ c ), which acts as a dimensionless activity number that balances the colloid size against the active nematic length scale a = K/α [54][55][56][57] and the ratio of drag coefficients γ /γ c . As such, activity introduces a radial potential whose slope depends on the angular position of the colloid.…”
Section: Colloid-defect Pair Dynamicsmentioning
confidence: 99%