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Liquid Crystals

Behavior of a Flexible Polymer in Solution in the Isotropic Phase of a Nematic Liquid Crystal

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Pages 135-149 | Received 20 Oct 1988, Accepted 04 Nov 1988, Published online: 04 Oct 2006

References

  • Dubault , A. , Casagrande , C. and Veyssie , M. 1982 . Mol. Cryst. Liq. Cryst. Lett. , 72 : 189
  • Dubault , A. , Casagrande , C. and Veyssie , M. 1978 . Mol. Cryst. Liq. Cryst. Lett. , 41 : 239
  • Dubault , A. , Casagrande , C. , Veyssie , M. and Deloche , B. 1980 . Phys. Rev. Lett. , 45 : 1645
  • Dubault , A. , Ober , R. , Veyssie , M. and Cabane , B. 1985 . J. Physique , 46 : 1227
  • Martinoty , P. , Dubault , A. , Casagrande , C. and Veyssie , M. 1983 . J. Physique Lettre , 44 : 935
  • de Gennes , P. G. 1971 . Mol. Cryst. Liq. Cryst. , 12 : 193 “The Physics of Liquid Crystals” Oxford University Press, London (1974)
  • Dunmur , D. A. and Tomes , A. E. 1981 . Mol. Cryst. Liq. Cryst. , 76 : 231
  • Filippini , J. C. and Poggi , Y. 1974 . J. Physique Lettres , 35 : 99 Physics Letters 49A, 291 (1974)
  • Bischofberger , T. , Yu , R. and Shen , Y. R. 1977 . Mol. Cryst. Liq. Cryst. , 43 : 287
  • Bird , R. B. , Hassager , O. , Armstrong , R. C. and Curtiss , C. F. 1977 . “ Dynamics of Polymeric Liquid ” . In Kinetic Theory , Vol. II , Wiley .
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  • de Gennes , P. G. 1974 . “The Physics of Liquid Crystals” , 174 London : Oxford University Press . e ≃ (Kd/η)1/3 where K is an elastic constant, η the viscosity and d the diameter of the capillary
  • For MBBA α1 = 6.5 cP, ηc = 121 cP at T = 25°C (see Reference 12)
  • Brochard , F. 1979 . C. R. Acad. Sc. Paris , 289B : 229
  • Brochard , F. 1980 . C. R. Acad. Sci. Paris , 290 B : 485
  • de Gennes , P. G. 1979 . Scaling Concepts in Polymer Physics , Ithaca : Cornell Univ. Press . P. Flory, Principles of Polymer Chemistry, Cornell Univ. Press, Ithaca 8th printing (1971)
  • These two values of a can, however, be seen to be slightly different, whereas estimation from the n = 1/a 3 relationship gives a ≃ 7.5 Å for both solvents. This slight difference could be explained by the fact that the ratio (Δn)0 (Δε)0/[nbar] may not be the same for the mixture and the pure solvent, which is not the assumption we made
  • Rao , N. V. S. , Kishore , P. R. , Raj , T. F. S. , Avadhanlu , M. N. and Marty , C. R. K. 1976 . Mol. Cryst. Liq. Cryst. , 36 : 65
  • Dubault , A. 1981 . Thesis Paris
  • Stinson , T. W. and Ulster , J. D. 1973 . Phys. Rev. Lett. , 30 : 688
  • Coles , H. J. and Jennings , B. R. 1978 . Molec. Phys. , 36 : 1661
  • de Gennes , P. G. 1984 . Mol. Cryst. Liq. Cryst. Lett. , 102 : 95
  • Ferry , J. 1970 . 230 London : Viscoelastic Properties of Polymers, Wiley . The first characteristic time of the coil can be estimated by extrapolating the results reported by, for polystyrenes with molecular weights of 82 000, 267 000 and 860 000. The characteristic time thus obtained is of the order of 10−7 − 10−8 sec. The life time T of the local nematic order is of the order of 10−7 sec near the transition (see Ref. 22)
  • Kiry , F. and Martinoty , P. 1977 . J. Physique , 38 : 153

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