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Volumn 53, Issue 2, 1996, Pages 1805-1815

Cell dynamics model of droplet formation in polymer-dispersed liquid crystals

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0006827584     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.53.1805     Document Type: Article
Times cited : (17)

References (72)
  • 5
    • 85035236154 scopus 로고    scopus 로고
    • Here it is assumed that the LC material has positive dielectric anisotropy. Reverse mode operation, where the PDLC is transparent in the ``off'' state and opaque in the ``on'' state, is also possible. This requires LCs with negative dielectric anisotropy and is relevant to some of the potential applications listed. See Ref. 4 for details.
    • Here it is assumed that the LC material has positive dielectric anisotropy. Reverse mode operation, where the PDLC is transparent in the ``off'' state and opaque in the ``on'' state, is also possible. This requires LCs with negative dielectric anisotropy and is relevant to some of the potential applications listed. See Ref. 4 for details.
  • 15
    • 0004178866 scopus 로고    scopus 로고
    • Phase Transformations
    • H. L. Anderson (American Society for Metals, Metals Park, OH 1970
    • J. E. Hilliard, in Phase Transformations, edited by H. L. Anderson (American Society for Metals, Metals Park, OH 1970).
    • Hilliard, J.E.1
  • 20
    • 0003544037 scopus 로고
    • Scaling Concepts in Polymer Physics
    • Cornell University Press, Ithaca
    • P. G. de Gennes, Scaling Concepts in Polymer Physics (Cornell University Press, Ithaca, 1979).
    • (1979)
    • de Gennes, P.G.1
  • 22
    • 85035210121 scopus 로고    scopus 로고
    • All PDLCs seem to have upper critical solution points Ref. 19.
    • All PDLCs seem to have upper critical solution points Ref. 19.
  • 31
    • 0003480237 scopus 로고
    • Phase Transitions and Critical Phenomena
    • C. Domb and J. L. Lebowitz Academic, London
    • See, e.g., J. D. Gunton, M. San Miguel, and P. S. Sahni, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, London, 1983), Vol. 8, pp. 267 466.
    • (1983) , vol.8 , pp. 267-466
    • Gunton, J.D.1    San Miguel, M.2    Sahni, P.S.3
  • 36
    • 85035221714 scopus 로고    scopus 로고
    • chemically more realistic models, the reaction would not be governed by contact of monomer molecules with the network, but with radical groups. These are either dissociated activators or activated polymer molecules, leading a more or less ``ghostly'' existence [H. M. J. Boots (private communication)].
    • In chemically more realistic models, the reaction would not be governed by contact of monomer molecules with the network, but with radical groups. These are either dissociated activators or activated polymer molecules, leading a more or less ``ghostly'' existence [H. M. J. Boots (private communication)].
  • 37
    • 0004213121 scopus 로고
    • On Growth and Form
    • H. E. Stanley and N. Ostrowsky Nijhof, Dordrecht
    • See, e.g., On Growth and Form, edited by H. E. Stanley and N. Ostrowsky (Nijhof, Dordrecht, 1985).
    • (1985)
  • 40
    • 0003605397 scopus 로고
    • Directions in Condensed Matter Physics
    • G. Grinstein and G. Mazenko World Scientific, Philadelphia
    • J. S. Langer, in Directions in Condensed Matter Physics, edited by G. Grinstein and G. Mazenko (World Scientific, Philadelphia, 1986), pp. 164 186.
    • (1986) , pp. 164 186
    • Langer, J.S.1
  • 46
    • 0003474751 scopus 로고
    • Numerical Recipes: The Art of Scientific Computing, 2nd ed.
    • Cambridge University Press, Cambridge
    • W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes: The Art of Scientific Computing, 2nd ed. (Cambridge University Press, Cambridge, 1992).
    • (1992)
    • Press, W.H.1    Teukolsky, S.A.2    Vetterling, W.T.3    Flannery, B.P.4
  • 51
    • 85035219978 scopus 로고    scopus 로고
    • See Ref. 44Ref. 45Ref. 47Ref. 48Ref. 49 for the relationship between partial differential equation and CDS models.
    • See Ref. 44 Ref. 45 Ref. 47 Ref. 48 Ref. 49 for the relationship between partial differential equation and CDS models.
  • 58
    • 0001475209 scopus 로고
    • but standard scaling for any finite n [A. J. Bray and K. Humayun, Phys. Rev. Lett. 68, 1559 (1992)
    • Care should be exercised when extrapolating to finite n, though. A classic example is the Cahn Hilliard equation, which exhibits multiscaling of the structure factor in the limit n = ∞ [A. Coniglio and M. Zanetti, Europhys. Lett. 10, 575 (1989)], but standard scaling for any finite n [A. J. Bray and K. Humayun, Phys. Rev. Lett. 68, 1559 (1992)].
    • (1989) Europhys. Lett. , vol.10 , pp. 575
    • Coniglio, A.1    Zanetti, M.2    Bray, A.J.3    Humayun, K.4
  • 64
    • 85035206854 scopus 로고    scopus 로고
    • See, e.g., D. Stauffer, Introduction to Percolation Theory (Taylor & Francis, London, 1985), p. 17.
    • See, e.g., D. Stauffer, Introduction to Percolation Theory (Taylor & Francis, London, 1985), p. 17.
  • 65
    • 85035218021 scopus 로고    scopus 로고
    • This is indeed seen in our model, for [Formula Presented] sim 0.2 0.3.
    • This is indeed seen in our model, for ψ0 sim 0.2 0.3.
  • 67
    • 0003499994 scopus 로고
    • Solids Far From Equilibrium
    • C. Godrèche Cambridge University Press, Cambridge
    • J. S. Langer, in Solids Far From Equilibrium, edited by C. Godrèche (Cambridge University Press, Cambridge, 1992), pp. 297 363.
    • (1992) , pp. 297 363
    • Langer, J.S.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.