Formation of shish-like fibril crystals from the melt of blends of cyclic and linear polyethylene under shear flow

The role of chain entanglements in shear-induced crystallization is one of the most important unsolved problems. The entanglements formed by topologically distinct cyclic and linear polymers are particularly notable. The shear-induced crystallization behavior of a blend of cyclic polyethylene (C-PE)...

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Bibliographic Details
Published inPolymer journal Vol. 54; no. 7; pp. 913 - 920
Main Authors Kobayashi, Keiko, Yamazaki, Shinichi, Kimura, Kunio
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 01.07.2022
Nature Publishing Group
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Summary:The role of chain entanglements in shear-induced crystallization is one of the most important unsolved problems. The entanglements formed by topologically distinct cyclic and linear polymers are particularly notable. The shear-induced crystallization behavior of a blend of cyclic polyethylene (C-PE) and linear polyethylene (L-PE) was investigated. Using C-PE as a matrix and L-PE as an additive, we changed the molecular weight and blend ratio of C-PE and L-PE and measured the formation rate of shish-like fibril crystals, I . In both blend systems of C-PE(230k)/L-PE(42k) and C-PE(230k)/L-PE(104k), where the values in parentheses represent the molecular weight, I reached a maximum at a certain weight fraction of L-PE, Φ L-PE . As the Φ L-PE was increased, that is, the entanglement density was increased, the formation of the oriented melt was promoted while crystallization was simultaneously suppressed by entanglements. The maximum value of I was observed owing to these two competing factors. Similar behavior was observed in the blend systems of C-PE(230k)/L-PE(42k), C-PE(130k)/L-PE(42k), and C-PE(86k)/L-PE(42k). The shear-induced crystallization behavior of the blends of cyclic polyethylene (C-PE) and linear polyethylene (L-PE) was investigated. This figure shows the formation rate of shish-like fibril crystals ( I ) in the blend systems of C-PE(230k)/L-PE(42k) and C-PE(230k)/L-PE(104k) against the weight fraction of L-PE, Φ L-PE . I reached a maximum at a certain Φ L-PE . As Φ L-PE increased, that is, as the entanglement density increased, the formation of the oriented melt was promoted. Crystallization was also suppressed by the entanglements. The maximum value of I was observed owing to these two competing factors.
ISSN:0032-3896
1349-0540
DOI:10.1038/s41428-022-00643-x