2015
DOI: 10.1007/s00707-015-1490-4
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Transient growth of a micro-void in an infinite medium under thermal load with modified Zerilli–Armstrong model

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Cited by 5 publications
(2 citation statements)
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“…It is suitable to predict the flow behavior of a large amount of materials at different strain rates and temperatures, which range from room temperature to 0.6 T m ( T m is the melting temperature). Baghani et al [43] considered the temperature-dependent behavior and used a modified Z–A model to describe the plastic hardening characteristics over a wide range of temperature. Mirzaie et al [44] modified the Z–A model by taking into account both a hardening and a softening effect to predict the hot flow stress of materials.…”
Section: Introductionmentioning
confidence: 99%
“…It is suitable to predict the flow behavior of a large amount of materials at different strain rates and temperatures, which range from room temperature to 0.6 T m ( T m is the melting temperature). Baghani et al [43] considered the temperature-dependent behavior and used a modified Z–A model to describe the plastic hardening characteristics over a wide range of temperature. Mirzaie et al [44] modified the Z–A model by taking into account both a hardening and a softening effect to predict the hot flow stress of materials.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the Arrhenius equation cannot accurately describe the flow stress, nor can it be sufficiently coupled with the microstructural evolution. The Zerilli–Armstrong and Johnson–Cook equations are also widely used, but they are unable to accurately track the deformation behavior within an entire temperature range and strain rate, especially during the tangible softening stage . Meanwhile, they also fail to account for the coupled influence of strain rate, strain, temperature, and microstructure.…”
Section: Introductionmentioning
confidence: 99%