2019
DOI: 10.5346/trbane.2019.39
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A Study on the Unification of the Threshold Stress Intensity Factor for Micro Crack Growth

Abstract: When the crack length is larger than a certain size, the maximum stress intensity factor (Kmax) is used to explain the occurrence condition of brittle crack, and the limit condition of hydrogen assisted and stress corrosion crack propagation. Also, the fatigue crack can be explained by the stress intensity factor range (ΔK). However, since the stress intensity factor deals with only linear elastic body, it is necessary for nonlinear range of crack tip to be small enough. It is known that in the case where this… Show more

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Cited by 16 publications
(25 citation statements)
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“…4 ΔK R th l ð Þ of a large crack is constant, but ΔK R th s ð Þ of a small crack decreases as the crack becomes shorter. These phenomena have been found in the brittle fracture 5 and hydrogen embrittlement of metals 6 and ceramics. 7,8 This is because a large crack satisfies smallscale yielding conditions (small-scale nonlinear region conditions, in the case of ceramics), but a small crack does not.…”
Section: Introductionmentioning
confidence: 85%
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“…4 ΔK R th l ð Þ of a large crack is constant, but ΔK R th s ð Þ of a small crack decreases as the crack becomes shorter. These phenomena have been found in the brittle fracture 5 and hydrogen embrittlement of metals 6 and ceramics. 7,8 This is because a large crack satisfies smallscale yielding conditions (small-scale nonlinear region conditions, in the case of ceramics), but a small crack does not.…”
Section: Introductionmentioning
confidence: 85%
“…Following the Milne et al method, 5 the small crack problem of high-strength steel under critical stress that causes hydrogen embrittlement of can be clearly explained. 6 Structural ceramics are typical brittle materials that exhibit small crack behaviour. The Milne et al method 5 was used to clarify this behaviour.…”
Section: Infinite Plate With a Through Crack Of Length (2l)mentioning
confidence: 99%
“…When Equations 2 and 3 are applied to a semielliptical crack in a finite plate, the equivalent crack length ( l e ) given by Equation 4 and is substituted in l in Equations 2 and 3 21,22 πle=βAπa, where a is the depth of the semielliptical crack and β A is the shape correction factor given by the Newman–Raju equation 28 at the deepest crack part (point A ) when the specimen of the finite plate is subjected to a bending stress.…”
Section: Analysis Methods and Detection Probability Of Fatigue Crackmentioning
confidence: 99%
“…When Equations 2 and 3 are applied to a semielliptical crack in a finite plate, the equivalent crack length (l e ) given by Equation 4 and is substituted in l in Equations 2 and 3. 21,22 ffiffiffiffiffiffi…”
Section: Analysis Methodsmentioning
confidence: 99%
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