Abstract:When dispersed in thermotropic nematic liquid crystal oils, surfactant-ladden aqueous droplets often lead to the formation of a equatorial ring disclination in the nearby nematic matrix as a result of a balance between elasticity and interfacial energy. In this experimental work, the aqueous phase contains an extract of cytoskeletal proteins that self-assemble into an active quasi-two-dimensional shell featuring self-sustained periodic flows. The ensuing hydrodynamic coupling drives the surrounding liquid crys… Show more
“…From the precedent considerations, it is clear that active nematic emulsions, the active counterparts of the nematic emul- Referring to the LC encapsulation of the microtubule/kinesin active material, the obvious question to be addressed is the eventual coupling between the active defects driving cortical flows inside the droplets and the passive singularities sitting around them in the surrounding passive LC. We analyzed this question in a couple of recent contributions published by Guillamat et al [24], and Hardoüin et al [25]. We briefly review on what follows the most paradigmatic scenario as reported in [24].…”
Section: Active Nematic Emulsionsmentioning
confidence: 97%
“…The mentioned variety of observed behaviors is likely to be due to both a quite wide range of droplet size distribution, added to the difficulty to guarantee a uniform partition of the components of the active sample and of the chemical surfactant. More details can be found in the paper published by Hardoüin et al [25].…”
“…From the precedent considerations, it is clear that active nematic emulsions, the active counterparts of the nematic emul- Referring to the LC encapsulation of the microtubule/kinesin active material, the obvious question to be addressed is the eventual coupling between the active defects driving cortical flows inside the droplets and the passive singularities sitting around them in the surrounding passive LC. We analyzed this question in a couple of recent contributions published by Guillamat et al [24], and Hardoüin et al [25]. We briefly review on what follows the most paradigmatic scenario as reported in [24].…”
Section: Active Nematic Emulsionsmentioning
confidence: 97%
“…The mentioned variety of observed behaviors is likely to be due to both a quite wide range of droplet size distribution, added to the difficulty to guarantee a uniform partition of the components of the active sample and of the chemical surfactant. More details can be found in the paper published by Hardoüin et al [25].…”
“…5a and b). [63][64][65][66][67][68][69][70][71] During one semi-period, the defects move from a tetrahedral configuration to a planar one or vice versa. For larger |a| values, such an oscillatory motion is inherited by the shell itself, which, again by virtue of the mechanical coupling between defects and curvature, periodically deforms from spherical to elliptical (Fig.…”
Section: Protrusion Formation In Nematic Shellsmentioning
Recent experimental observations have suggested that topological defects can facilitate the cre- ation of sharp features in developing embryos. Whereas these observations echo established knowledge about the interplay between geometry...
“…For instance, they facilitate self-assembly and the formation of metamaterials [28,29], and enable novel control of topological defects [27,30,31]. While there have been studies of active nematic droplets in a host passive liquid crystal [32,33], colloidal inclusions in host active nematics have not been looked at previously.…”
We introduce a general description of localised distortions in active nematics using the framework of active nematic multipoles. We give the Stokesian flows for arbitrary multipoles in terms of differentiation of a fundamental flow response and describe them explicitly up to quadrupole order. We also present the response in terms of the net active force and torque associated to the multipole. This allows the identification of the dipolar and quadrupolar distortions that generate self-propulsion and self-rotation respectively and serves as a guide for the design of arbitrary flow responses. Our results can be applied to both defect loops in three-dimensional active nematics and to systems with colloidal inclusions. They reveal the geometry-dependence of the self-dynamics of defect loops and provide insights into how colloids might be designed to achieve propulsive or rotational dynamics, and more generally for the extraction of work from active nematics. Finally, we extend our analysis also to two dimensions and to systems with chiral active stresses.
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