Young and Young-Laplace equations for a static ridge of nematic liquid crystal, and transitions between equilibrium states

Motivated by the need for greater understanding of systems that involve interfaces between a nematic liquid crystal, a solid substrate and a passive gas that include nematic-substrate-gas three-phase contact lines, we analyse a two-dimensional static ridge of nematic resting on a solid substrate in...

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Bibliographic Details
Main Authors: Cousins, J.R.L (Author), Duffy, B.R (Author), Mottram, N.J (Author), Wilson, S.K (Author)
Format: Article
Language:English
Published: Royal Society Publishing 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02555nam a2200433Ia 4500
001 10.1098-rspa.2021.0849
008 220425s2022 CNT 000 0 und d
020 |a 13645021 (ISSN) 
245 1 0 |a Young and Young-Laplace equations for a static ridge of nematic liquid crystal, and transitions between equilibrium states 
260 0 |b Royal Society Publishing  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1098/rspa.2021.0849 
520 3 |a Motivated by the need for greater understanding of systems that involve interfaces between a nematic liquid crystal, a solid substrate and a passive gas that include nematic-substrate-gas three-phase contact lines, we analyse a two-dimensional static ridge of nematic resting on a solid substrate in an atmosphere of passive gas. Specifically, we obtain the first complete theoretical description for this system, including nematic Young and Young-Laplace equations, and then, making the assumption that anchoring breaking occurs in regions adjacent to the contact lines, we use the nematic Young equations to determine the continuous and discontinuous transitions that occur between the equilibrium states of complete wetting, partial wetting and complete dewetting. In particular, in addition to continuous transitions analogous to those that occur in the classical case of an isotropic liquid, we find a variety of discontinuous transitions, as well as contact-angle hysteresis, and regions of parameter space in which there exist multiple partial wetting states that do not occur in the classical case. © 2022 The Authors. 
650 0 4 |a Contact angle 
650 0 4 |a Continuous transitions 
650 0 4 |a dewetting 
650 0 4 |a De-wetting 
650 0 4 |a Discontinuous transition 
650 0 4 |a Equilibrium state 
650 0 4 |a Integrodifferential equations 
650 0 4 |a Laplace equation 
650 0 4 |a Laplace transforms 
650 0 4 |a nematic liquid crystals 
650 0 4 |a Nematic liquid crystals 
650 0 4 |a Nematics 
650 0 4 |a Partial wetting 
650 0 4 |a Phase interfaces 
650 0 4 |a Solid substrates 
650 0 4 |a wetting 
650 0 4 |a Wetting 
650 0 4 |a Young equation 
650 0 4 |a Young Laplace equation 
650 0 4 |a Young-Laplace equation 
650 0 4 |a Young's equation 
650 0 4 |a Young's-Laplace equation 
700 1 |a Cousins, J.R.L.  |e author 
700 1 |a Duffy, B.R.  |e author 
700 1 |a Mottram, N.J.  |e author 
700 1 |a Wilson, S.K.  |e author 
773 |t Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences