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Helix reversals as bad neighbors to liquid crystal organizations in cholesteric states and thermally reversible gels of poly(ALKYL isocyanates)
Author(s) -
Green Mark M.,
Khatri Chetan,
Mark Herman F.
Publication year - 1994
Publication title -
macromolecular symposia
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.257
H-Index - 76
eISSN - 1521-3900
pISSN - 1022-1360
DOI - 10.1002/masy.19940770129
Subject(s) - liquid crystal , isocyanate , helix (gastropod) , alkyl , materials science , lyotropic , chirality (physics) , crystallography , lyotropic liquid crystal , supramolecular chemistry , cholesteric liquid crystal , polymer chemistry , phase (matter) , phase diagram , chemical physics , chemistry , organic chemistry , crystal structure , liquid crystalline , polyurethane , composite material , chiral symmetry breaking , snail , ecology , biology , quark , quantum mechanics , nambu–jona lasinio model , physics , optoelectronics
While the temperature dependence of the lyotropic cholesteric pitch of the single helical sense poly ((R)‐2,6‐dimethylheptyl isocyanate) is in line with theory, comparable data on this state produced by chiral doping of the lyotropic nematic state of poly(n‐hexyl isocyanate) could suggest an interplay between the supramolecular chirality of the liquid crystal and the dynamic equilibrium of the left and right hand helical blocks in this otherwise racemic polyisocyanate. The exclusion of helix reversals, as undersireable kinks in the liquid crystal organization, could play a role in this effect. Such helix reversal exclusions can also explain the peculiar chiral optical changes associated with the thermally reversible gelation of poly(n‐hexyl isocyanate) copolymers in hydrocarbon solvents. These gels likely arise by entering the broad biphasic region of the Flory phase diagram leading to the formation of liquid crystal aggregates.