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Rheology of polyphosphazene melts and solutions—some surprises
Author(s) -
Ho Perry K.,
Williams Michael C.
Publication year - 1981
Publication title -
polymer engineering and science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.503
H-Index - 111
eISSN - 1548-2634
pISSN - 0032-3888
DOI - 10.1002/pen.760210410
Subject(s) - rheology , thermodynamics , materials science , superposition principle , shear rate , rheometer , viscosity , polymer , relaxation (psychology) , rheometry , arrhenius equation , polymer chemistry , physics , chemistry , activation energy , composite material , psychology , social psychology , quantum mechanics
Abstract Rheological tests are reported for two types of polyorganophosphazenes, one being a fluorinated alkoxy terpolymer (PNFT) and the other an aryloxy copolymer (PAP). Non‐Newtonian viscosity η( \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm \dot \gamma } $\end{document} ) and complex viscosity components η′(ω) and η″(ω) were measured as functions of shear rate \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm \dot \gamma } $\end{document} and oscillatory frequency ω, using a Weissenberg rheogoniometer, and a limited amount of normal stress data was also obtained. Solutions of both polymers in tetrahydrofuran were tested, over a concentration range 0‐22 percent for PNFT and 0‐35 percent for PAP. Melts of PNFT were examined for temperatures 50‐178°C, and melts of PAP at 210°C even though they were not truly fluid at this temperature. Solution and melt data are shown to obey conventional superposition principles to give master curves. For solutions, superposition is achieved by using the Bueche relaxation time as a concentration reducing factor with no adjustable parameters, and the Spriggs model also proves useful in predicting normal stress and shear stress results. For PNFT melts, master curves are fitted by the new WS 2 H 2 model which incorporates detailed molecular weight distribution (MWD) information and extracts the entanglement length M e from the data. Temperature shift factors a T show Arrhenius behavior and the corresponding activation energies E re are reported. Results for PNFT melts were complicated by lack of agreement between two samples of nominally the same composition; η′(ω) shapes and levels and E re values differed widely. This is interpreted in terms of detailed MWD information and the possibility of mesomorphic phase transitions occurring in these nominally amorphous materials.