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Rheological properties of liquid crystalline solutions of ethyl celluloses with different molecular weight in m ‐cresol
Author(s) -
Suto Shinichi,
Ohshiro Masahiko,
Nishibori Wataru,
Tomita Hisashi,
Karasawa Mikio
Publication year - 1988
Publication title -
journal of applied polymer science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.575
H-Index - 166
eISSN - 1097-4628
pISSN - 0021-8995
DOI - 10.1002/app.1988.070350210
Subject(s) - shear rate , viscoelasticity , materials science , rheology , rheometer , liquid crystal , thermodynamics , shear (geology) , composite material , physics , optoelectronics
Steady‐state shear rheological properties of liquid crystalline solutions of four ethyl celluloses (ECs) were determined at a low shear rate (1 s −1 ) and at relatively high shear rates by using two rheometers (cone‐plate and capillary types), and were compared with those of liquid crystalline hydroxypropyl cellulose (HPC). The effect of molecular weight (MW) on the viscoelastic behavior was also determined. The viscoelastic behavior was also determined. The viscometric behavior of EC solutions was similar to that of HPC solutions: (1) with respect to temperature, the shear viscosity (η) at shear rate of 1 s −1 exhibited a minimum (η min ) and a maximum (η max ), and the concentration–temperature superposition for η could be applied; (2) the behavior of η at relatively high shear rates as a function of shear rate or polymer concentration was typical of lyotropic liquid crystals. The MW dependence of η min was greater than that of η max for EC solutions. The behavior of the elastic parameters such as Bagley correction factor ( v ), entrance pressure drop (Δ P ent ), and die swell ( B ) at relatively high shear rates for EC solutions was essentially similar to that for HPC solutions: (1) the shear rate or stress dependence of the elastic parameters was greatly dependent on whether the polymer solution was in a single phase or biphase; (2) with respect to concentration the elastic parameters showed a maximum and a minimum and the maximum or minimum point for each parameter was not always identical to each other. η for the isotropic or fully anisotropic solutions at a given concentration ( C ) increased, whereas η for the solutions in the vicinity of the biphasic region showed a minimum, with respect to MW. The slope of η at a given shear rate vs. C M w depended on shear rate, and this slope for the isotropic solutions appeared to be greater than that for fully anisotropic solutions. Δ P ent and v at a given concentration showed either a monotonical increase or a maximum or minimum with MW, and this behavior was not fully consistent with that of η. B for the isotropic solutions increased and B 's for both biphasic and fully anisotropic solutions were almost constant, with MW.