Domain motion in confined liquid crystals
We extend a lattice Boltzmann algorithm of liquid crystal hydrodynamics to include an applied electric field. The approach solves the equations of motion written in terms of a tensor order parameter. Back-flow effects and the hydrodynamics of topological defects are included. We investigate some of...
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2002
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author | Denniston, C Toth, G Yeomans, J |
author_facet | Denniston, C Toth, G Yeomans, J |
author_sort | Denniston, C |
collection | OXFORD |
description | We extend a lattice Boltzmann algorithm of liquid crystal hydrodynamics to include an applied electric field. The approach solves the equations of motion written in terms of a tensor order parameter. Back-flow effects and the hydrodynamics of topological defects are included. We investigate some of the dynamics relevant to liquid crystal devices; in particular defect-mediated motion of domain walls relevant to the nucleation of states useful in pi-cells. An anisotropy in the domain wall velocity is seen because defects of different topology couple differently to the flow field. |
first_indexed | 2024-03-06T21:13:28Z |
format | Conference item |
id | oxford-uuid:3ef6c38d-a704-4e52-9135-87aa393cfa4d |
institution | University of Oxford |
last_indexed | 2024-03-06T21:13:28Z |
publishDate | 2002 |
record_format | dspace |
spelling | oxford-uuid:3ef6c38d-a704-4e52-9135-87aa393cfa4d2022-03-26T14:29:01ZDomain motion in confined liquid crystalsConference itemhttp://purl.org/coar/resource_type/c_5794uuid:3ef6c38d-a704-4e52-9135-87aa393cfa4dSymplectic Elements at Oxford2002Denniston, CToth, GYeomans, JWe extend a lattice Boltzmann algorithm of liquid crystal hydrodynamics to include an applied electric field. The approach solves the equations of motion written in terms of a tensor order parameter. Back-flow effects and the hydrodynamics of topological defects are included. We investigate some of the dynamics relevant to liquid crystal devices; in particular defect-mediated motion of domain walls relevant to the nucleation of states useful in pi-cells. An anisotropy in the domain wall velocity is seen because defects of different topology couple differently to the flow field. |
spellingShingle | Denniston, C Toth, G Yeomans, J Domain motion in confined liquid crystals |
title | Domain motion in confined liquid crystals |
title_full | Domain motion in confined liquid crystals |
title_fullStr | Domain motion in confined liquid crystals |
title_full_unstemmed | Domain motion in confined liquid crystals |
title_short | Domain motion in confined liquid crystals |
title_sort | domain motion in confined liquid crystals |
work_keys_str_mv | AT dennistonc domainmotioninconfinedliquidcrystals AT tothg domainmotioninconfinedliquidcrystals AT yeomansj domainmotioninconfinedliquidcrystals |