1987
DOI: 10.1115/1.3173053
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Introduction to Continuum Damage Mechanics

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Cited by 122 publications
(106 citation statements)
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“…In general, damage accumulation can occur under elastic deformation (fatigue), elastic-plastic deformation (ductile plastic damage), or under creep conditions (creep damage). In more complex cases, d can assume the form of a vector function or fourth order tensor (Kachanov, 1986). Here, we assume the simple case where d is a scalar function of the equivalent plastic strains.…”
Section: Resultsmentioning
confidence: 99%
“…In general, damage accumulation can occur under elastic deformation (fatigue), elastic-plastic deformation (ductile plastic damage), or under creep conditions (creep damage). In more complex cases, d can assume the form of a vector function or fourth order tensor (Kachanov, 1986). Here, we assume the simple case where d is a scalar function of the equivalent plastic strains.…”
Section: Resultsmentioning
confidence: 99%
“…In anisotropic cases of non-random crack orientations, it should be changed to a symmetric second rank crack density tensor [10]:…”
Section: Spherical Pores and Circular Or Elliptical Cracksmentioning
confidence: 99%
“…Based on basic damage mechanics (Kachanov, 1986, Lemaitre, 1996), the microdamage density ( D ) can be simply defined as follows: D=1EiE0 where E i is the instantaneous modulus and E 0 is the original modulus.…”
Section: Empirical Constitutive Relationshipsmentioning
confidence: 99%
“…Kachanov’s damage model states that damage evolves as a power law function of the effective stress (Kachanov, 1986). Krajcinovic et al (Krajcinovic, et al, 1987) proposed a linear elastic damage model using a simple statistical mode of fiber pull-out.…”
Section: Introductionmentioning
confidence: 99%