Related Experiment Videos
Telephone-cord instabilities in thin smectic capillaries
Paolo Biscari1, Maria Carme Calderer
1Dipartimento di Matematica, Politecnico di Milano, P. Leonardo da Vinci 32, 20133 Milan, Italy. paolo.biscari@polimi.it
Summary
Spontaneous polarization drives telephone-cord patterns in liquid-crystal capillaries. This instability leads to curved and helicoidal capillary shapes in Smectic-A* and Smectic-C* phases, respectively, revealing new liquid crystal phenomena.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Soft Matter Physics
Background:
- Telephone-cord patterns, a novel instability, have been observed in smectic liquid-crystal capillaries.
- Understanding the physical mechanisms driving these complex structures is crucial for materials science and physics.
Purpose of the Study:
- To analyze the factors inducing telephone-cord patterns in smectic liquid-crystal capillaries.
- To investigate the role of chiral pitch, bending stress, and spontaneous polarization in capillary shape transitions.
Main Methods:
- Theoretical analysis of free energy minimization in liquid-crystal phases.
- Modeling of capillary shape under various physical conditions, including spontaneous polarization and molecular tilt.
Main Results:
- A nonzero chiral cholesteric pitch favors the Smectic-A* to Smectic-C* transition in linear capillaries.
- Neither cholesteric pitch nor bending stress alone can induce capillary curvature.
- Spontaneous polarization is identified as the key factor for the telephone-cord instability, leading to nonzero capillary curvature in the Sm-A* phase.
- In the Sm-C* phase, molecular tilt and spontaneous polarization together induce a helicoidal capillary shape with curvature and torsion.
Conclusions:
- Spontaneous polarization is the essential driver for telephone-cord instability in liquid-crystal capillaries.
- The Sm-A* phase exhibits planar capillary shapes with curvature due to spontaneous polarization.
- The Sm-C* phase displays helicoidal capillary shapes, characterized by curvature and torsion, resulting from the interplay of molecular tilt and spontaneous polarization.