TY - JOUR
T1 - Bridging a mesoscopic inhomogeneity to macroscopic performance of amorphous materials in the framework of the phase field modeling
AU - Avalos, Edgar
AU - Xie, Shuangquan
AU - Akagi, Kazuto
AU - Nishiura, Yasumasa
N1 - Funding Information:
This work was partially supported by the Council for Science, Technology and Innovation (CSTI), Japan , Cross-ministerial Strategic Innovation Promotion Program (SIP), Japan , ‘Structural Materials for Innovation’ and ‘Materials Integration’ for Revolutionary Design System of Structural Materials. Also Y.N. gratefully acknowledges the support of KAKENHI, Japan Grants-in-Aid no. 18H05482 and the Fusion Research and Advanced Target Project of WPI AIMR, Tohoku University. Special thanks go to Professor Takeshi Takaishi (Musashino University) for providing us a code of the phase field model.
Publisher Copyright:
© 2020 Elsevier B.V.
PY - 2020/8
Y1 - 2020/8
N2 - One of the big challenges in materials science is to bridge microscopic or mesoscopic properties to macroscopic performance such as fracture toughness. This is particularly interesting for the amorphous materials such as epoxy resins because their micro/meso structures are difficult to characterize so that any information connecting different scales would be extremely useful. At the process level the polymerization rate, which influences considerably the performance of materials, can be changed experimentally. However, it is known that the maximum toughness does not always appear at the maximum polymerization rate, which suggests that some differences in the micro/meso-scopic structure affect the macroscopic property behind. The goal of this article is to present a framework to bridge between a mesoscopic observation of X-ray CT images and the macroscopic criterion of fracture toughness computed via phase field modeling. First we map the X-ray images with different polymerization rates into several categories using different methods: one is singular value decomposition (SVD) and the other is persistent homology. Secondly we compute a crack propagation of each sample and evaluate a scalar value called the effective toughness (ET) via J-integral, which is one of the good candidates indicating a toughness of materials. It turns out that ET reflects the performance of each sample and consistent with the experimental results.
AB - One of the big challenges in materials science is to bridge microscopic or mesoscopic properties to macroscopic performance such as fracture toughness. This is particularly interesting for the amorphous materials such as epoxy resins because their micro/meso structures are difficult to characterize so that any information connecting different scales would be extremely useful. At the process level the polymerization rate, which influences considerably the performance of materials, can be changed experimentally. However, it is known that the maximum toughness does not always appear at the maximum polymerization rate, which suggests that some differences in the micro/meso-scopic structure affect the macroscopic property behind. The goal of this article is to present a framework to bridge between a mesoscopic observation of X-ray CT images and the macroscopic criterion of fracture toughness computed via phase field modeling. First we map the X-ray images with different polymerization rates into several categories using different methods: one is singular value decomposition (SVD) and the other is persistent homology. Secondly we compute a crack propagation of each sample and evaluate a scalar value called the effective toughness (ET) via J-integral, which is one of the good candidates indicating a toughness of materials. It turns out that ET reflects the performance of each sample and consistent with the experimental results.
KW - Amorphous materials
KW - Crack propagation
KW - Fracture toughness
KW - Persistent homology
KW - Phase field model
KW - Singular value decomposition
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U2 - 10.1016/j.physd.2020.132470
DO - 10.1016/j.physd.2020.132470
M3 - Article
AN - SCOPUS:85082706340
SN - 0167-2789
VL - 409
JO - Physica D: Nonlinear Phenomena
JF - Physica D: Nonlinear Phenomena
M1 - 132470
ER -