Topography from topology in liquid crystal elastomer coatings

ORAL

Abstract

Liquid crystal elastomer (LCE) free-standing films containing topological defects deform on heating into three-dimensional shapes [1-3]. Attaching such LCE films to a rigid substrate as a coating provides the opportunity to create temperature-responsive surface topography, a phenomenon demonstrated by Babakhanova et al [4]. Using finite element method (FEM) simulation, we model surface deformations produced by LCE coatings with defects as a function of both topological charge and orientational phase angle. We find that, on heating, a radial +1 defect produces an inward depression while a circular +1 produces an outward elevation. The -1 defect and higher order +/- integer defects produce wrinkle patterns with out-of-plane surface deformations. By contrast, +/- half-integer defects give rise to both out-of-plane and in-plane displacements. Theoretical calculations in the limit of small strain elasticity explain these results and are compared with both FEM simulation and experimental data. [1] McConney et al, Adv Mater 25, 5880 (2013); [2] Konya et al, Front Mater 3, 24 (2016); [3] Modes et al Phys Rev E 81, 060701R (2010); [4] Babakhanova et al Nat Commun 9, 456 (2018).

Presenters

  • Youssef Mosaddeghian Golestani

    Kent State University

Authors

  • Youssef Mosaddeghian Golestani

    Kent State University

  • Greta Babakhanova

    Kent State University, Chemical Physics Interdisciplinary Program, Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, OH 44242, USA

  • Michael P Varga

    Kent State University

  • Hao Yu

    Kent State University, Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, Ohio, 44242, USA, Advanced Materials and Liquid Crystal Institute and Chemical Physics Interdisciplinary Program, Kent State University, Advanced Materials and Liquid Crystal Institute, Kent State Univeristy

  • Jonathan Selinger

    Kent State University

  • Qi-Huo Wei

    Kent State University, Advanced Material and Liquid Crystal Institute, Kent State University, Kent, OH44242, Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, Ohio, 44242, USA, Advanced Materials and Liquid Crystal Institute and Chemical Physics Interdisciplinary Program and Physics Department, Kent State University, Advanced Materials and Liquid Crystal Institute, Kent State Univeristy

  • O D Lavrentovich

    Kent State University, Advanced Materials and Liquid Crystal Institute, Kent State University, Kent, Ohio, 44242, USA, Department of Physics and Advanced Materials Liquid Crystal Institute, Kent State University, Advanced Materials and Liquid Crystal Institute and Chemical Physics Interdisciplinary Program and Physics Department, Kent State University, Advanced Materials and Liquid Crystal Institute, Kent State Univeristy, Advanced Materials and Liquid Crystal Institute / Department of Physics, Kent State University, Kent, OH 44242, USA, Department of Physics, Advanced Materials and Liquid Crystal Institute, Chemical Physics Interdisciplinary Program, Kent State University

  • Robin Selinger

    Kent State University