2013
DOI: 10.1002/jgrb.50125
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High‐temperature deformation and recrystallization: A variational analysis and its application to olivine aggregates

Abstract: [1] We develop a framework for a variational analysis of microstructural evolution during inelastic high-temperature deformation accommodated by dislocation mechanisms and diffusive mass transport. A polycrystalline aggregate is represented by a distribution function characterizing the state of individual grains by three variables, dislocation density, grain size, and elastic strain. The aggregate's free energy comprises elastic energy and energies of lattice distortions due to dislocations and grain boundarie… Show more

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Cited by 18 publications
(27 citation statements)
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References 111 publications
(198 reference statements)
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“…We focus on the grain growth law reported by Karato (1989), the range of mobility presented in the review by Evans et al (2001), and a recent quantitative estimate derived from analyzing piezometric relations of olivine aggregates (Hackl and Renner, 2013). For the temperature range of our experiments a spread of 10 −18 to 10 −11 m 4 J −1 s −1 is indicated (Fig.…”
Section: Quantitative Analysismentioning
confidence: 84%
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“…We focus on the grain growth law reported by Karato (1989), the range of mobility presented in the review by Evans et al (2001), and a recent quantitative estimate derived from analyzing piezometric relations of olivine aggregates (Hackl and Renner, 2013). For the temperature range of our experiments a spread of 10 −18 to 10 −11 m 4 J −1 s −1 is indicated (Fig.…”
Section: Quantitative Analysismentioning
confidence: 84%
“…10a), likely due to a lower nucleus density and/or predominant occurrence of fragments. Furthermore, variations in the driving force for growth during isostatic annealing have to be considered for the recrystallized grains that are almost free of defects and for the fragments that inherit the deformed microstructure (see for example Hackl and Renner, 2013, for an analytic expression of the dependence of a grain's size evolution on the relation between its energy state and that of its environment). The driving force for growth of new grains, i.e., the difference in their free energy and that of their environment, G, is here simply associated with two defect concentrations, the density of interfaces (surface area per volume for a single grain, here represented by the inverse of grain size, i.e., a grain-shape dependent geometrical factor is neglected Solid Earth, 4, 423-450, 2013 www.solid-earth.net/4/423/2013/ for simplicity but can be considered to be included in the uncertainty of the specific interface energy) and the density of dislocations (length of dislocations per volume),…”
Section: Grain Size Evolution During Isostatic Annealingmentioning
confidence: 99%
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“…We investigate the mathematical model based on the work of Hackl and Renner [1] for the phenomenon of dynamic recrystallization in polycrystalline materials. In [1], a probability distribution function f (D, ρ) was introduced, where the state of individual grains is determined by grain size D and dislocation density ρ which we collect into the state variable x = (D, ρ).…”
Section: Mathematical Modelmentioning
confidence: 99%
“…In [1], a probability distribution function f (D, ρ) was introduced, where the state of individual grains is determined by grain size D and dislocation density ρ which we collect into the state variable x = (D, ρ). The distribution function has to satisfy the continuity equation:…”
Section: Mathematical Modelmentioning
confidence: 99%