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Development of the Cube Component \( \left( {\left\{ 001 \right\}\left\langle {100} \right\rangle } \right) \) During Plane Strain Compression of Copper and Its Importance in Recrystallization Nucleation

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Abstract

The origin of cube texture during recrystallization of medium to high stacking-fault energy FCC metals has been debated for several decades. However, the evolution of cube component during deformation is not studied well and hence, it is still unclear what are the favorable nucleation sites for the cube oriented recrystallized grains. To resolve this issue, we applied a full field crystal plasticity model utilizing a dislocation density based constitutive theory for the simulation of plane strain compression of polycrystalline copper. Simulation results reveal that the grains with initially cube orientation retained a small fraction of the cube component in the deformed state, whereas, some of the grains with initially non-cube orientations developed the cube component during the deformation. For strain up to 0.46, non-cube grains which are within 10 to 20 deg from the ideal cube orientation showed the highest tendency to develop the cube component during deformation. However, the cube component developed during the deformation was unstable and rotated away from the cube orientation with further deformation. With increasing strain up to 1.38, some of the grains with higher angular deviation from the ideal cube orientation also developed the cube component. No particular axis preference was observed for the non-cube grains, rather, the evolution of the cube component becomes dynamic at larger strain. Analysis of the disorientation angle and the dislocation density difference with the neighboring locations shows that the cube component developed during the deformation can play a significant role during nucleation. These findings will be useful for controlling the cube texture in FCC metals.

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Acknowledgments

The authors want to acknowledge the National Science Foundation, Division of Civil, Mechanical and Manufacturing Innovation for their support under the Grant No. CMMI-1662646. SC and CSP want to acknowledge the Simulation Innovation and Modeling Center, The Ohio State University and Ohio Supercomputer Center for providing computational resources. The authors also like to thank Prof. Anthony Rollett and Prof. Roger Doherty for valuable discussions.

Conflict of interest

The authors declare that they have no conflict of interest.

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Authors and Affiliations

  1. Department of Materials Science and Engineering, The Ohio State University, Columbus, OH, 43210, USA

    Supriyo Chakraborty, Chaitali S. Patil & Stephen R. Niezgoda

  2. Department of Mechanical and Aerospace Engineering, The Ohio State University, Columbus, OH, 43210, USA

    Stephen R. Niezgoda

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  1. Supriyo Chakraborty
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  2. Chaitali S. Patil
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Correspondence to Stephen R. Niezgoda.

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Manuscript submitted August 17, 2021, accepted October 23, 2021.

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Appendix

Appendix

See Fig. A1, Tables A1 and A2.

Table A1 Miller Indices and Euler Angles of the Main Texture Components[65,70]
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Table A2 Orientation of Grain G1, G2 and G3 and Their Corresponding Orientations in the Experiment
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Fig. A1
figure 16

ODF corresponding to the non-cube grains which developed the cube component at strain of \(\epsilon _{vM}\) = 1.38 in RVE M1, is presented in 2D sections of reduced Euler space. The \(\beta \)-fiber coordinates, as defined in the work of Sidor and Kestens,[76] are also shown using star shaped markers. Very low intensity around the \(\beta \)-fiber is clearly visible

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Chakraborty, S., Patil, C.S. & Niezgoda, S.R. Development of the Cube Component \( \left( {\left\{ 001 \right\}\left\langle {100} \right\rangle } \right) \) During Plane Strain Compression of Copper and Its Importance in Recrystallization Nucleation. Metall Mater Trans A 53, 503–522 (2022). https://doi.org/10.1007/s11661-021-06513-0

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