References
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- Martinoty , P. , Dubault , A. , Casagrande , C. and Veyssie , M. 1983 . J. Physique Lettre , 44 : 935
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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)
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- 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
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- Dubault , A. 1981 . Thesis Paris
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- 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