1998
DOI: 10.1023/a:1004371203514
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Cracking phenomena of brittle films in nanostructure composites analysed by a modified shear lag model with residual strain

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Cited by 102 publications
(57 citation statements)
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“…In the i + 1' increment the stress in the middle of the region of interest has exceeded the critical value for one of the cohesive zone elements, a new crack is generated, and the σ x x surface stresses go towards zero. This crack progression is consistent with the shear lag models for tensile cracking [Agrawal and Raj 1989;Wojciechowski and Mendolia 1989;Yanaka et al 1998;Chen et al 1999;2000]. From shear lag assumptions and from the above description of the contours in Figure 6, one would expect the cracks always to form at the midpoint between two adjacent cracks.…”
Section: Stress Distributionssupporting
confidence: 82%
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“…In the i + 1' increment the stress in the middle of the region of interest has exceeded the critical value for one of the cohesive zone elements, a new crack is generated, and the σ x x surface stresses go towards zero. This crack progression is consistent with the shear lag models for tensile cracking [Agrawal and Raj 1989;Wojciechowski and Mendolia 1989;Yanaka et al 1998;Chen et al 1999;2000]. From shear lag assumptions and from the above description of the contours in Figure 6, one would expect the cracks always to form at the midpoint between two adjacent cracks.…”
Section: Stress Distributionssupporting
confidence: 82%
“…However, this expectation is based on the assumption that the stress profile in Figure 6 is unchanged through the thickness of the coating. Uniform stresses along the thickness of the coating are also an underlying assumption in the analytical models referred to above [Agrawal and Raj 1989;Wojciechowski and Mendolia 1989;Yanaka et al 1998;Chen et al 1999;2000]. It was found that the stresses are not uniform through the coating thickness.…”
Section: Stress Distributionsmentioning
confidence: 99%
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