TY - JOUR
T1 - Observation of Crack Tip Strain Distribution for Brittle Materials by Means of Photoelastic Coating Technique and Non-Linear Fracture Mechanics
AU - Fukasawa, Takayuki
AU - Hashida, Toshiyuki
AU - Takahashi, Hideaki
N1 - Copyright:
Copyright 2016 Elsevier B.V., All rights reserved.
PY - 1988
Y1 - 1988
N2 - Granite, granite and mortar are typical brittle materials. Recently, for evaluating the strength of these materials, a study based on fracture mechanics has been suggested. In general a microcrack process zone at the crack tip of brittle materials is created, which may determine the fracture process. So using the photoelastic coating method with a PLZT (transparent dielectric ceramics) plate (100 -200 μm thickness), the strain field at the crack tip was directly measured. As a result, it was found that the strain field did not show the singularity of γ-1/2, (γ = a distance from crack tip), as the strain field of linear elastic materials. When the strain distributions are normalized by J integral and the tensile stress σull they were expressed by a form of Δɛ=Δɛ0 ((J/ σull/r)m; thus it is found that the strain field within the process zone can be described by the J integral, where Δɛ and m are material constants, and m is near 1. The strain field at the crack tip of the brittle materials is proportional to approximately γ-1. The extension of the process zone, denoted by ω, is closely related to the J integral. The relationship between ω and the J integral can be expressed as a bilinear line. It is shown that the J integral at the knee point is equal to the critical J integral, value determined by AE technique. Thus the J integral can be an important parameter to evaluate the fracture behavior of brittle materials.
AB - Granite, granite and mortar are typical brittle materials. Recently, for evaluating the strength of these materials, a study based on fracture mechanics has been suggested. In general a microcrack process zone at the crack tip of brittle materials is created, which may determine the fracture process. So using the photoelastic coating method with a PLZT (transparent dielectric ceramics) plate (100 -200 μm thickness), the strain field at the crack tip was directly measured. As a result, it was found that the strain field did not show the singularity of γ-1/2, (γ = a distance from crack tip), as the strain field of linear elastic materials. When the strain distributions are normalized by J integral and the tensile stress σull they were expressed by a form of Δɛ=Δɛ0 ((J/ σull/r)m; thus it is found that the strain field within the process zone can be described by the J integral, where Δɛ and m are material constants, and m is near 1. The strain field at the crack tip of the brittle materials is proportional to approximately γ-1. The extension of the process zone, denoted by ω, is closely related to the J integral. The relationship between ω and the J integral can be expressed as a bilinear line. It is shown that the J integral at the knee point is equal to the critical J integral, value determined by AE technique. Thus the J integral can be an important parameter to evaluate the fracture behavior of brittle materials.
KW - Brittle Material
KW - Crack Tip Strain Field
KW - Fracture
KW - J Integral
KW - Photoelastic Coating Technique
KW - Process Zone
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U2 - 10.1299/kikaia.54.1553
DO - 10.1299/kikaia.54.1553
M3 - Article
AN - SCOPUS:0024056597
VL - 54
SP - 1553
EP - 1558
JO - Nihon Kikai Gakkai Ronbunshu, A Hen/Transactions of the Japan Society of Mechanical Engineers, Part A
JF - Nihon Kikai Gakkai Ronbunshu, A Hen/Transactions of the Japan Society of Mechanical Engineers, Part A
SN - 0387-5008
IS - 504
ER -