Microstructure and mechanical response of single-crystalline high-manganese austenitic steels under high-pressure torsion: The effect of stacking-fault energy

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Authors

  • E. G. Astafurova
  • M. S. Tukeeva
  • G. G. Maier
  • E. V. Melnikov
  • H. J. Maier

Research Organisations

External Research Organisations

  • Siberian Branch of the Russian Academy of Sciences
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Details

Original languageEnglish
Pages (from-to)166-175
Number of pages10
JournalMaterials Science and Engineering A
Volume604
Publication statusPublished - 17 Mar 2014

Abstract

We investigate the kinetics of the structural deformation and hardening of single-crystalline austenitic Fe-13Mn-1.3C (Hadfield steel), Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C (in wt%) steels with different stacking-fault energies after cold high-pressure torsion. Independently of the stacking-fault energy, mechanical twinning was found to be the basic deformation mechanism responsible for the rapid generation of an ultrafine-grained microstructure with a high volume fraction of twin boundaries. Under high-pressure torsion, the spacing between twin boundaries increases, and the dislocation density and microhardness decrease as the stacking-fault energy increases. The formation of a twin net from the beginning of plastic flow in Fe-13Mn-1.3C steel provides a homogeneous distribution of microhardness values across the discs independent of strain under torsion. Lower hardness values in the disk centers compared to the periphery were observed for the two other steels, Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C, with higher stacking-fault energies due to changes in the densities of the twin boundaries. An additional increase in the dislocation density for the Fe-13Mn-1.3C steel was detected compared with the Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C steels, which was a result of torsion in the temperature range of dynamic strain aging. The appearance of small fractions of ε and α' phases in the structures of the Fe-13Mn-1.3C, Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C steels is discussed.

Keywords

    Austenite, High-pressure torsion, Microstructure, Stacking-fault energy, Steel, Twinning

ASJC Scopus subject areas

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Microstructure and mechanical response of single-crystalline high-manganese austenitic steels under high-pressure torsion: The effect of stacking-fault energy. / Astafurova, E. G.; Tukeeva, M. S.; Maier, G. G. et al.
In: Materials Science and Engineering A, Vol. 604, 17.03.2014, p. 166-175.

Research output: Contribution to journalArticleResearchpeer review

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title = "Microstructure and mechanical response of single-crystalline high-manganese austenitic steels under high-pressure torsion: The effect of stacking-fault energy",
abstract = "We investigate the kinetics of the structural deformation and hardening of single-crystalline austenitic Fe-13Mn-1.3C (Hadfield steel), Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C (in wt%) steels with different stacking-fault energies after cold high-pressure torsion. Independently of the stacking-fault energy, mechanical twinning was found to be the basic deformation mechanism responsible for the rapid generation of an ultrafine-grained microstructure with a high volume fraction of twin boundaries. Under high-pressure torsion, the spacing between twin boundaries increases, and the dislocation density and microhardness decrease as the stacking-fault energy increases. The formation of a twin net from the beginning of plastic flow in Fe-13Mn-1.3C steel provides a homogeneous distribution of microhardness values across the discs independent of strain under torsion. Lower hardness values in the disk centers compared to the periphery were observed for the two other steels, Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C, with higher stacking-fault energies due to changes in the densities of the twin boundaries. An additional increase in the dislocation density for the Fe-13Mn-1.3C steel was detected compared with the Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C steels, which was a result of torsion in the temperature range of dynamic strain aging. The appearance of small fractions of ε and α' phases in the structures of the Fe-13Mn-1.3C, Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C steels is discussed.",
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note = "Funding information: The authors wish to thank Professor Y. Chumlyakov for providing the single crystals and for fruitful discussions. This research was partially supported by the Russian Ministry of Education and Science (Contract no. 8749 , 01.10.2012) and Russian President Scholarship (SP-4384.2013.1).",
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TY - JOUR

T1 - Microstructure and mechanical response of single-crystalline high-manganese austenitic steels under high-pressure torsion

T2 - The effect of stacking-fault energy

AU - Astafurova, E. G.

AU - Tukeeva, M. S.

AU - Maier, G. G.

AU - Melnikov, E. V.

AU - Maier, H. J.

N1 - Funding information: The authors wish to thank Professor Y. Chumlyakov for providing the single crystals and for fruitful discussions. This research was partially supported by the Russian Ministry of Education and Science (Contract no. 8749 , 01.10.2012) and Russian President Scholarship (SP-4384.2013.1).

PY - 2014/3/17

Y1 - 2014/3/17

N2 - We investigate the kinetics of the structural deformation and hardening of single-crystalline austenitic Fe-13Mn-1.3C (Hadfield steel), Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C (in wt%) steels with different stacking-fault energies after cold high-pressure torsion. Independently of the stacking-fault energy, mechanical twinning was found to be the basic deformation mechanism responsible for the rapid generation of an ultrafine-grained microstructure with a high volume fraction of twin boundaries. Under high-pressure torsion, the spacing between twin boundaries increases, and the dislocation density and microhardness decrease as the stacking-fault energy increases. The formation of a twin net from the beginning of plastic flow in Fe-13Mn-1.3C steel provides a homogeneous distribution of microhardness values across the discs independent of strain under torsion. Lower hardness values in the disk centers compared to the periphery were observed for the two other steels, Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C, with higher stacking-fault energies due to changes in the densities of the twin boundaries. An additional increase in the dislocation density for the Fe-13Mn-1.3C steel was detected compared with the Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C steels, which was a result of torsion in the temperature range of dynamic strain aging. The appearance of small fractions of ε and α' phases in the structures of the Fe-13Mn-1.3C, Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C steels is discussed.

AB - We investigate the kinetics of the structural deformation and hardening of single-crystalline austenitic Fe-13Mn-1.3C (Hadfield steel), Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C (in wt%) steels with different stacking-fault energies after cold high-pressure torsion. Independently of the stacking-fault energy, mechanical twinning was found to be the basic deformation mechanism responsible for the rapid generation of an ultrafine-grained microstructure with a high volume fraction of twin boundaries. Under high-pressure torsion, the spacing between twin boundaries increases, and the dislocation density and microhardness decrease as the stacking-fault energy increases. The formation of a twin net from the beginning of plastic flow in Fe-13Mn-1.3C steel provides a homogeneous distribution of microhardness values across the discs independent of strain under torsion. Lower hardness values in the disk centers compared to the periphery were observed for the two other steels, Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C, with higher stacking-fault energies due to changes in the densities of the twin boundaries. An additional increase in the dislocation density for the Fe-13Mn-1.3C steel was detected compared with the Fe-13Mn-2.7Al-1.3C and Fe-28Mn-2.7Al-1.3C steels, which was a result of torsion in the temperature range of dynamic strain aging. The appearance of small fractions of ε and α' phases in the structures of the Fe-13Mn-1.3C, Fe-13Mn-2.7Al-1.3C, and Fe-28Mn-2.7Al-1.3C steels is discussed.

KW - Austenite

KW - High-pressure torsion

KW - Microstructure

KW - Stacking-fault energy

KW - Steel

KW - Twinning

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U2 - 10.1016/j.msea.2014.03.029

DO - 10.1016/j.msea.2014.03.029

M3 - Article

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VL - 604

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EP - 175

JO - Materials Science and Engineering A

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ER -

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