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Dynamic x-ray diffraction studies of high-density polyethylene
Authors:Robert J. Cembrola  Thein Kyu  Richard S. Stein  Shoji Suehiro  Hiromichi Kawai
Abstract:Dynamic x-ray diffraction is conducted to explore the structural origin of the α and β mechanical dispersions of a melt-crystallized high-density polyethylene. It is shown that the real component of the strain orientation coefficient for the crystal c axis Curn:x-wiley:00981273:media:POL180210302:tex2gif-stack-1 decreases with increasing frequency at a rate which decreases with decreasing temperature. Values of Curn:x-wiley:00981273:media:POL180210302:tex2gif-stack-2 for the c axis are positive, Curn:x-wiley:00981273:media:POL180210302:tex2gif-stack-3 for the a axis negative, and Curn:x-wiley:00981273:media:POL180210302:tex2gif-stack-4 for the b axis close to zero, suggesting that the predominant relaxation process is crystal rotation about the b axis. The activation energy found from Arrhenius plots of Curn:x-wiley:00981273:media:POL180210302:tex2gif-stack-5 corresponds to that of the α1 mechanical dispersion. The dynamic birefringence in this region is dominated by the contribution from crystal orientation changes. At low temperatures, the imaginary component KCurn:x-wiley:00981273:media:POL180210302:tex2gif-stack-6 of the strain-optical coefficient of the crystal phase approaches zero, while KCurn:x-wiley:00981273:media:POL180210302:tex2gif-stack-7 of the amorphous phase exhibits a somewhat broad dispersion peak corresponding to the β birefringence dispersion. This suggests that the principal contribution to the β birefringence dispersion arises from the amorphous phase, probably owing to the amorphous orientation process. Contrary to the case of low-density polyethylene, the dynamic crystal lattice deformation and compliance functions reveal distinct frequency dispersions corresponding to the α1 and α2 mechanical processes. The α1 lattice dispersion is thought to be associated with the α1 crystal orientation dispersion, while the α2 lattice dispersion is believed to be the inherent one arising from the onset of intracrystalline chain motions.
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