Hostname: page-component-78c5997874-94fs2 Total loading time: 0 Render date: 2024-11-10T22:01:24.620Z Has data issue: false hasContentIssue false

Characterising texture formation in fibre lattices embedded in a nematic liquid crystal matrix

Published online by Cambridge University Press:  28 January 2011

P. M. PHILLIPS
Affiliation:
Department of Chemical Engineering, McGill University, Montreal, Quebec, CanadaH3A 2B2 e-mail: paul.phillips@mail.mcgill.ca
A. D. REY
Affiliation:
Department of Chemical Engineering, McGill University, Montreal, Quebec, CanadaH3A 2B2 e-mail: paul.phillips@mail.mcgill.ca

Abstract

A two-dimensional computational study is performed on the texturing of fibre-filled nematic liquid crystals using the Landau-de Gennes model describing the spatio-temporal evolution of the second moment of the orientation distribution function or quadrupolar tensor order parameter. The investigation is performed on a consistent computational domain comprising a square array of four circular fibres embedded within a unit square containing a uniaxial low molar mass calamitic liquid crystal. Interest is focused on the role of temperature, boundary conditions and their effect on the nucleation and evolution of defect structures. Thermal effects are characterised below and above the temperature at which the nematic state is stable. Simulations in the stable nematic state serves as a scenario for investigating the effect of imposing different external boundary conditions, namely periodic and Dirichlet; the former describes a square lattice array of fibres embedded in a nematic liquid crystal, and the latterdescribes a four-fibre arrangement in an aligned nematic material. In each case, the influence of temperature is characterised, with defect structures forming and either remaining or splitting into lower strength defects. For fibre lattices, splitting transitions of defects at the centre of the domain occur at a critical temperature, but for the four-fibre arrangement, defect transitions occur continuously over a temperature range. The discontinuous defect splitting transition in fibre arrays occurs at lower temperatures than the continuous defect transformation in the four-fibre arrangement. At sufficiently low temperatures, the four-fibre arrangement and the fibre lattice give the same texture consisting of two disclination lines close to each fibre. The evolution of the texture with respect to temperature can be characterised as a change from single-fibre mode at low temperature to a collective mode with a centre-located heterogeneity at higher temperature. At higher temperatures, in the stable isotropic state, it is shown that surface-induced ordering arising from the fibre/liquid crystal interaction propagates into the bulk forming thin disclination lattices around the four-fibre configuration.

Type
Papers
Copyright
Copyright © Cambridge University Press 2011

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

[1]Araki, T., Tojo, K., Furukawa, A. & Onuki, A. (2009) Defect structures in nematic liquid crystals around charged particles. Eur. Phys. J. 30, 5564.Google Scholar
[2]Brandac, Z., Svetec, M., Kralij, S. & Zumer, S. (2006) Anhilation of nematic point defects: Pre-collision and post-collision evolution. Eur. Phys. J. 20, 7179.Google Scholar
[3]Chandrasekhar, S. (1986) The structures and energetics of defects in liquid crystals. Adv. Phys. 35, 507596.CrossRefGoogle Scholar
[4]Coles, J. H. (1978) Laser and electric field induced birefringence studies on cyanobphenyl homologs. Mol. Cryst. Liq. Cryst. 49, 6774.CrossRefGoogle Scholar
[5]COMSOL. (1998) Multiphysics, modelling and simulation [online]. URL: http:/www.comsol.com.Google Scholar
[6]de Andrade Lima, L. R. P., Grecov, D. & Rey, D. A. (2006) Multiscale theory and simulation for fiber precursors based on carbonaceous mesophases. Plast., Rubbers Compos. 35, 276286.Google Scholar
[7]de Gennes, P. G. & Prost, J. (1993) The Physics of Liquid Crystals, Clarendon, Oxford.CrossRefGoogle Scholar
[8]de Luca, G. & Rey, D. A. (2007) Point and ring defects under capillary confinement. J. Chem. Phys. 127 (104902), 111.CrossRefGoogle ScholarPubMed
[9]de Luca, G. & Rey, D. A. (2007) Ring-like cores of cylindrically confined nematic point defects. J. Chem. Phys. 126 (094907), 111.CrossRefGoogle Scholar
[10]Friedel, J. (1967) Dislocations. Pergamon, Oxford.Google Scholar
[11]Fukuda, J. & Yokoyama, H. (2001) Direct configuration and dynamics of a nematic liquid crystal around a two dimensional spherical particle: Numerical analysis using adaptive grids. Eur. Phys. J. 4, 389396.Google Scholar
[12]Grecov, D. & Rey, D. A. (2006) Texture control strategies for flow-aligning liquid crystal polymers. J. Non-Newton. Fluid Mech. 139, 197208.CrossRefGoogle Scholar
[13]Gupta, G. & Rey, D. A. (2005) Texture modeling in carbon–carbon composites based on mesophase precursor matrices. Carbon 43, 14001406.CrossRefGoogle Scholar
[14]Gupta, G. & Rey, D. A. (2005) Texture rules for filled nematics. Phys. Rev. Lett. 95 (127802), 14.CrossRefGoogle ScholarPubMed
[15]Hess, S. & Sonnet, A. (1995) Alignment tensors versus director: Description of defects in nematic liquid crystals. Phys. Rev. 52, 718722.Google Scholar
[16]Hogan, J. S. & Mottram, J. N. (1997) Disclination core structure and induced phase change in nematic liquid crystals. Phil. Trans. Soc. 355, 20452064.Google Scholar
[17]Hwang, K. D., Gupta, G. & Rey, D. A. (2005) Optical and structural modeling of disclination lattices in carbonaceous mesophases. J. Chem. Phys. 122 (034902), 111.Google Scholar
[18]Kim, W. M., Boamfa, I. M. & Rasing, H. T. (2003) Observation of surface and bulk phase transitions in nematic liquid crystals. Nature 421, 149152.Google Scholar
[19]Kleman, M. (1982) Points, Lines and Walls: In Liquid Crystals, Magnetic Systems and Various Ordered Media, John Wiley and Sons, New York.Google Scholar
[20]Kleman, M. & Lavrentovichm, D. O. (2009) Soft Matter Physics: An Introduction, Springer Wien, New York.Google Scholar
[21]Mottram, J. N. & Sluckin, J. T. (2000) Defect-induced melting in nematic liquid crystals. Liq. Cryst. 10, 13011304.CrossRefGoogle Scholar
[22]Neyts, K., Baets, R. & Desmet, H. (2005) Modeling nematic liquid crystals in the neighborhood of edges. J. Appl. Phys. 98 (123517), 16.Google Scholar
[23]Noble-Luginbuhl, A. R., Blanchard, R. M. & Nuzzo, R. G. (2000) Surface effects on the dynamics of liquid crystalline thin films in nanoscale cavities. J. Am. Chem. Soc. 122, 39173926.CrossRefGoogle Scholar
[24]Oswald, P. & Pieranski, P. (2005) Nematic and Cholesteric Liquid Crystals: Concepts and Physical Properties Illustrated by Experiments, Taylor and Francis, New York.CrossRefGoogle Scholar
[25]Rey, D. A. (1995) Bifurcational analysis of the isotropic-nematic phase transition of rigid rod polymers subjected to biaxial stretching flow. Macromol. Theory Simul. 4, 857872.CrossRefGoogle Scholar
[26]Rey, D. A. (1995) Macroscopic theory of orientation transitions in the extension flow of side-chain nematic polymers. Rheol. Acta 34, 119131.CrossRefGoogle Scholar
[27]Rey, D. A. (2007) Capillary models for liquid crystal fibers, membranes, films and drops. Soft Matter 3, 13491368.CrossRefGoogle ScholarPubMed
[28]Rey, D. A. & Yan, J. (2003) Modelling elastic and viscous effects on the texture of ribbon shaped carbon fibers. Carbon 41, 105121.Google Scholar
[29]Schiele, K. & Trimper, S. (1983) On the elastic constants of a nematic liquid crystal. Phys. Stat. Sol. (b) 118, 267274.CrossRefGoogle Scholar
[30]Schopol, N. & Sluckin, J. T. (2007) Landau-de Gennes theory of isotropic–nematic–smectic liquid crystal transitions. Phys. Rev. Lett. 75 (051707), 111.Google Scholar
[31]Sokolovska, G. T., Sokolovskii, O. R. & Patey, N. G. (2004) Surface induced ordering of nematics in an external field: The strong influence of tilted walls. Phys. Rev. Lett. 92 (185508), 14.CrossRefGoogle Scholar
[32]Weitz, L. R. & Zimmer, E. J. (1984) Disclinations in a graphite fiber bundle. Carbon 22, 209.Google Scholar
[33]Wincure, B. & Rey, D. A. (2006) Heterogeneous curved moving nematic–isotropic fronts. J. Chem. Phys. 124 (244902), 113.CrossRefGoogle Scholar
[34]Wincure, B. & Rey, D. A. (2007) Computational modeling of nematic phase ordering by film and droplet growth over heterogeneous substrates. Liq. Cryst. 34, 13971413.CrossRefGoogle Scholar
[35]Wincure, B. & Rey, D. A. (2007) Growth and structure of nematic spherulites under shallow thermal quenches. Contin. Mech. Thermodyn. 19, 3758.CrossRefGoogle Scholar
[36]Wincure, B. & Rey, D. A. (2007) Nanoscale analysis of defect shedding from liquid crystal interfaces. Nano. Lett. 7, 14741479.CrossRefGoogle ScholarPubMed
[37]Yan, J. & Rey, D. A. (2002) Texture formation in carbonaceous mesophase fibers. Phys. Rev. 65 (031713), 114.Google ScholarPubMed