Higher order twin modes in martensitic NiTi: The (201̄) case

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  • University of Illinois Urbana-Champaign (UIUC)
  • Universität Paderborn
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Details

OriginalspracheEnglisch
Seiten (von - bis)422-430
Seitenumfang9
FachzeitschriftMaterials Science and Engineering A
Jahrgang558
PublikationsstatusVeröffentlicht - 14 Aug. 2012
Extern publiziertJa

Abstract

NiTi alloys in the martensitic phase deform by detwinning of the martensite variants succeeded by deformation twinning of the single crystal of martensite. One of the deformation twinning modes of the martensite is denoted as (20. 1-)[. 1-0. 2-]. In this work, we establish how twinning on the (20. 1-) planes develops via the combination of homogeneous shear and shuffle and establish its energy barrier via atomistic simulations. We calculate the slip barrier in addition to the twin barrier ruling out the potential for plastic flow via slip in the (20. 1-) plane. The (20. 1-)[. 1-0. 2-] mode succeeds the (001) and (100) compound twinning modes which have lower energy barriers. It plays a significant role in allowing deformation to higher strains in the martensitic phase. Therefore, the insight into the (20. 1-)[. 1-0. 2-] twinning mode is important in extending the shape memory strains in NiTi alloys and towards better understanding of shape memory alloys in general.

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Higher order twin modes in martensitic NiTi: The (201̄) case. / Ezaz, T.; Sehitoglu, H.; Abuzaid, W. et al.
in: Materials Science and Engineering A, Jahrgang 558, 14.08.2012, S. 422-430.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Ezaz T, Sehitoglu H, Abuzaid W, Maier HJ. Higher order twin modes in martensitic NiTi: The (201̄) case. Materials Science and Engineering A. 2012 Aug 14;558:422-430. doi: 10.1016/j.msea.2012.08.022
Ezaz, T. ; Sehitoglu, H. ; Abuzaid, W. et al. / Higher order twin modes in martensitic NiTi : The (201̄) case. in: Materials Science and Engineering A. 2012 ; Jahrgang 558. S. 422-430.
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abstract = "NiTi alloys in the martensitic phase deform by detwinning of the martensite variants succeeded by deformation twinning of the single crystal of martensite. One of the deformation twinning modes of the martensite is denoted as (20. 1-)[. 1-0. 2-]. In this work, we establish how twinning on the (20. 1-) planes develops via the combination of homogeneous shear and shuffle and establish its energy barrier via atomistic simulations. We calculate the slip barrier in addition to the twin barrier ruling out the potential for plastic flow via slip in the (20. 1-) plane. The (20. 1-)[. 1-0. 2-] mode succeeds the (001) and (100) compound twinning modes which have lower energy barriers. It plays a significant role in allowing deformation to higher strains in the martensitic phase. Therefore, the insight into the (20. 1-)[. 1-0. 2-] twinning mode is important in extending the shape memory strains in NiTi alloys and towards better understanding of shape memory alloys in general.",
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T2 - The (201̄) case

AU - Ezaz, T.

AU - Sehitoglu, H.

AU - Abuzaid, W.

AU - Maier, H. J.

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PY - 2012/8/14

Y1 - 2012/8/14

N2 - NiTi alloys in the martensitic phase deform by detwinning of the martensite variants succeeded by deformation twinning of the single crystal of martensite. One of the deformation twinning modes of the martensite is denoted as (20. 1-)[. 1-0. 2-]. In this work, we establish how twinning on the (20. 1-) planes develops via the combination of homogeneous shear and shuffle and establish its energy barrier via atomistic simulations. We calculate the slip barrier in addition to the twin barrier ruling out the potential for plastic flow via slip in the (20. 1-) plane. The (20. 1-)[. 1-0. 2-] mode succeeds the (001) and (100) compound twinning modes which have lower energy barriers. It plays a significant role in allowing deformation to higher strains in the martensitic phase. Therefore, the insight into the (20. 1-)[. 1-0. 2-] twinning mode is important in extending the shape memory strains in NiTi alloys and towards better understanding of shape memory alloys in general.

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