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Published on: December 4, 2014
Shaping thin nematic films with competing boundary conditions
1Nordita, Royal Institute of Technology & Stockholm University, Roslagstullsbacken 23, SE-10691, Stockholm, Sweden, oksanam@nordita.org.
Free liquid crystal films become unstable at a threshold thickness, transitioning from flat to patterned structures. This study reveals how elastic anisotropy drives these shape changes in nematic liquid crystals.
Area of Science:
- Soft Matter Physics
- Materials Science
- Liquid Crystal Physics
Background:
- Free interfaces of liquid crystals naturally minimize capillarity and anchoring forces.
- Understanding the interplay between liquid crystal order and interface deformation is crucial for materials with free interfaces.
Purpose of the Study:
- To investigate the coupling between director configuration and free interface shape in nematic films.
- To determine the threshold thickness for instability in planar and radial geometries with antagonistic anchoring.
- To analyze the formation of patterned structures due to elastic anisotropy.
Main Methods:
- Utilizing a perturbation ansatz to model director configurations and interface shapes.
- Analytical investigation in the long-wavelength limit, independent of surface tension.
- Quantifying bifurcations in circular ring geometries.
Main Results:
- An analytical threshold thickness was found for the instability of flat nematic films.
- The study quantifies the bifurcation of circular rings into structures with m-fold rotational symmetry.
- Elastic anisotropy of the bulk nematic director was identified as the driving force for pattern formation.
Conclusions:
- The simplified approach provides insights into elastic and capillary phenomena in liquid crystalline materials.
- The findings are relevant for understanding the behavior of materials with inherent liquid crystalline order and deformable interfaces.
- This work contributes to the fundamental understanding of pattern formation driven by elastic and capillary effects.
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