TY - JOUR
T1 - Specific deformation behavior of isotactic polypropylene films under a multiaxial stress field
AU - Kojio, Ken
AU - Fujimoto, Aya
AU - Nagano, Chigusa
AU - Nozaki, Shuhei
AU - Yokomachi, Kazutoshi
AU - Kamitani, Kazutaka
AU - Watanabe, Hirohmi
AU - Takahara, Atsushi
N1 - Funding Information:
This work was supported by the Impulsing Paradigm Change through Disruptive Technology (ImPACT) Program, Japan Science and Technology Agency, PRESTO, Grant Number JPMJPR2194, JSPS KAKENHI Grant Number 21H02003. Synchrotron radiation X-ray scattering measurements were performed at BL05XU, BL40XU, and BL20XU in the SPring-8 facility with the approval of the Japan Synchrotron Radiation Research Institute (JASRI; Proposal No. 2016A1414, 2016B1436, 2015B1459, 2018B1035, 2019A1015, 2019B1011, 2021A1452). We gratefully acknowledge Dr Taiki Hoshino, Dr So Fujinami, Dr Tomotaka Nakatani, Mr Kohki Aoyama, and Dr Akihisa Takeuchi for their assistance with the WAXD and SAXS measurements.
Publisher Copyright:
© 2022 The Royal Society of Chemistry
PY - 2022/4/4
Y1 - 2022/4/4
N2 - The specific deformation behavior of crystalline polymer films, namely unoriented crystallized isotactic polypropylene (it PP) films, was investigated under a multiaxial stress field. Changes in the aggregation structure of the films were investigated during the bulge deformation process using in situ small-angle X-ray scattering, wide-angle X-ray diffraction (WAXD) measurements, and polarized high-speed-camera observations. The films had a thickness of approximately 10 μm. The it PP films were fixed at the hole of a plate, then bulge deformation was applied using N2 or He gas pressure, and stress-strain curves were then calculated from the applied pressure and bulge height. Yielding was observed in the stress-strain curves. Below the yield point, in situ WAXD measurements revealed that the crystal lattice expanded isotropically at the center, edge, and bottom of the bulge hole. Above the yield point, a craze started to form slightly near the center, and crazes formed in various directions with a further increase in strain, while the crystal lattice expanded uniaxially along the circumference at the edge and bottom. Crazes oriented in various directions merged and lost birefringence, indicating a change to the isotropic orientation. The different directions of the crazes indicated several directions of stress. In other words, even if multiaxial deformation is applied to a crystalline it PP film, the string-shaped crystalline polymer chain structure produces local anisotropic uniaxial stress.
AB - The specific deformation behavior of crystalline polymer films, namely unoriented crystallized isotactic polypropylene (it PP) films, was investigated under a multiaxial stress field. Changes in the aggregation structure of the films were investigated during the bulge deformation process using in situ small-angle X-ray scattering, wide-angle X-ray diffraction (WAXD) measurements, and polarized high-speed-camera observations. The films had a thickness of approximately 10 μm. The it PP films were fixed at the hole of a plate, then bulge deformation was applied using N2 or He gas pressure, and stress-strain curves were then calculated from the applied pressure and bulge height. Yielding was observed in the stress-strain curves. Below the yield point, in situ WAXD measurements revealed that the crystal lattice expanded isotropically at the center, edge, and bottom of the bulge hole. Above the yield point, a craze started to form slightly near the center, and crazes formed in various directions with a further increase in strain, while the crystal lattice expanded uniaxially along the circumference at the edge and bottom. Crazes oriented in various directions merged and lost birefringence, indicating a change to the isotropic orientation. The different directions of the crazes indicated several directions of stress. In other words, even if multiaxial deformation is applied to a crystalline it PP film, the string-shaped crystalline polymer chain structure produces local anisotropic uniaxial stress.
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U2 - 10.1039/d2sm00147k
DO - 10.1039/d2sm00147k
M3 - Article
C2 - 35416238
AN - SCOPUS:85129490528
SN - 1744-683X
VL - 18
SP - 3369
EP - 3375
JO - Soft Matter
JF - Soft Matter
IS - 17
ER -