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Dynamic Recrystallization in Cu-Cr-Zr-Ti Alloy Under Large Plane Strain Conditions

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dc.contributor.author SARKAR, A
dc.contributor.author MURTY, SVSN
dc.contributor.author PRASAD, MJNV
dc.date.accessioned 2021-03-10T07:45:34Z
dc.date.available 2021-03-10T07:45:34Z
dc.date.issued 2020
dc.identifier.citation METALLURGICAL AND MATERIALS TRANSACTIONS A-PHYSICAL METALLURGY AND MATERIALS SCIENCE 51(9)4742-4752 en_US
dc.identifier.issn 1073-5623
dc.identifier.issn 1543-1940
dc.identifier.uri https://doi.org/10.1007/s11661-020-05892-0
dc.identifier.uri http://localhost:8080/xmlui/handle/100/27585
dc.description.abstract The Cu-Cr-Zr-Ti alloy was subjected to single-hit plane strain compression tests in the temperature range of 923 K to 1073 K (650 degrees C to 800 degrees C) and at two different strain rates of 0.1 and 1 s(-1). These tests were performed to ascertain the kinetics of microstructural evolution resulting by dynamic recrystallization (DRX) in the alloy under hot deformation conditions. The differences in the extent of DRX under various deformation conditions were established by plotting fractional softening as a function of strain and time. Further, the Avrami exponent was found to decrease with increase in deformation temperature. This was attributed to early onset of recrystallization leading to subsequent work hardening of the recrystallized grains and grain growth at higher temperatures which results in the loss of nucleation sites due to reduced grain boundary area. Microstructural observations made using optical microscopy, scanning electron microscopy (SEM), and electron backscattered diffraction (EBSD) revealed nucleation to occur in the following steps: elongation of grains perpendicular to the compression direction, bulging of elongated grain boundaries due to strain-induced boundary migration (SIBM), and subsequent subgrain formation behind the bulged boundary due to strain-induced low-angle boundaries. Finally, the equation describing the DRX kinetics under plane strain conditions for the alloy was established as X = 1 - exp [-0.455 x ((epsilon - epsilon(c))/epsilon(p))(2.84)]. en_US
dc.language.iso English en_US
dc.publisher SPRINGER en_US
dc.subject HOT DEFORMATION en_US
dc.subject BEHAVIOR en_US
dc.subject MICROSTRUCTURE en_US
dc.subject TEMPERATURE en_US
dc.subject EVOLUTION en_US
dc.title Dynamic Recrystallization in Cu-Cr-Zr-Ti Alloy Under Large Plane Strain Conditions en_US
dc.type Article en_US


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