1999
DOI: 10.1016/s0020-7683(98)00239-x
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A void–crack nucleation model for ductile metals

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Cited by 190 publications
(86 citation statements)
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“…By inhibiting any of these three stages, the ductility and strength of these alloys can be improved. The process of void nucleation is fairly well understood by both experiment and theory [37][38][39][40][41]. Void nucleation usually occurs at second phase precipitates or inclusions.…”
Section: (A) Microdamage Evolution In Ductile Fracturementioning
confidence: 99%
“…By inhibiting any of these three stages, the ductility and strength of these alloys can be improved. The process of void nucleation is fairly well understood by both experiment and theory [37][38][39][40][41]. Void nucleation usually occurs at second phase precipitates or inclusions.…”
Section: (A) Microdamage Evolution In Ductile Fracturementioning
confidence: 99%
“…Schematic of the fictitious material with increasing nucleation density and void growth of a model framework The void nucleation rule follows the work done by Horstemeyer and Gohkale (1999) and is employed to capture the effect of voids nucleating under tension, compression, and torsion. The void nucleation function in the integrated form is given by, where coeff C is a material constant, T is temperature, ) (t ε is the strain rate, and T C η is a temperature dependent material constant.…”
Section: Damage Model Formulationmentioning
confidence: 99%
“…The internal state variable (ISV) plasticity-damage model presented by Bammann and Aifantis (1989) and Bammann et al (1996) and later modified to account for nucleation, growth, and coalescence by Horstemeyer and Gohkale (1999) and Horstemeyer et al, (2000) has been used to predict the plastic deformation of many types of metals under various loading conditions (cf. Horstemeyer, 2001).…”
Section: Introductionmentioning
confidence: 99%
“…(a) increasing void growth (b) increasing nucleation sites The void nucleation rule of Horstemeyer and Gokhale (1998) T is temperature in the absolute scale, and C Tη is the temperature dependent material constant determined from experiments ( Figure 3.19). The material parameters a, b, and c relate to the volume fraction of nucleation events arising from local microstresses in the material.…”
Section: -6mentioning
confidence: 99%