Spherical nematic shells with a prolate ellipsoidal core

被引:13
|
作者
Sadati, Monirosadat [1 ,2 ]
Zhou, Ye [1 ]
Melchert, Drew [1 ,3 ]
Guo, Ashley [1 ]
Martinez-Gonzalez, Jose A. [1 ,2 ,4 ]
Roberts, Tyler F. [1 ]
Zhang, Rui [1 ]
de Pablo, Juan J. [1 ,2 ]
机构
[1] Univ Chicago, Inst Mol Engn, Chicago, IL 60637 USA
[2] Argonne Natl Lab, Lemont, IL 60439 USA
[3] Univ Calif Santa Barbara, Mat Dept, Santa Barbara, CA 93106 USA
[4] Univ Autonoma San Luis Potosi, Lateral Av Salvador Nava S-N, San Luis Potosi 78290, Mexico
基金
美国国家科学基金会;
关键词
LIQUID-CRYSTAL; TOPOLOGICAL DEFECTS; DROPLETS; COLLOIDS; CONFIGURATIONS; INTERFACES; PARTICLES;
D O I
10.1039/c7sm01403a
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Liquid crystal shells have attracted considerable attention in recent years. In such systems, a combination of confinement and curvature generates topological defect structures that do not exist in the bulk. Past studies, however, have largely focused on perfectly spherical shells, and little attention has been devoted to the impact of core geometry on the configuration and arrangement of topological defects. In this work, a microfluidic glass capillary device is used to encapsulate spherical and prolate ellipsoidal particles in nematic liquid crystal (LC) droplets dispersed in aqueous media. Our experimental studies show that, when trapped inside a radial LC droplet, spherical particles with both homeotropic and planar anchoring are highly localized at the droplet's center. While the radial configuration of the LC droplets is not altered by a homeotropic particle, polystyrene particles with strong planar anchoring disturb the radial ordering, leading to a twisted structure. Experiments indicate that off-center particle positions can also arise, in which defects are displaced towards the vicinity of the droplet's surface. In contrast, when prolate ellipsoidal particles are encapsulated in a thick radial LC shell, the minimum free energy corresponds to configurations where the particle is positioned at the droplet center. In this case, defects arise at the two ends of the prolate ellipsoid, where the curvature of the particle is maximal, leading to the formation of peculiar hybrid and twisted structures.
引用
收藏
页码:7465 / 7472
页数:8
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