Energetics of (1 1 4) twinning in B2 NiTi under coupled shear and shuffle

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

Externe Organisationen

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

OriginalspracheEnglisch
Seiten (von - bis)339-348
Seitenumfang10
FachzeitschriftActa materialia
Jahrgang60
Ausgabenummer1
PublikationsstatusVeröffentlicht - 4 Nov. 2011
Extern publiziertJa

Abstract

The (1 1 4) twin growth in the austenitic regime in NiTi (B2 lattice) is characterized precisely at the atomistic scale. This twinning mode is consistent with experimental observations but has not been well understood despite its importance. Combined shears, shuffles and interface shifts operate in a complex way to generate the (1 1 4) twin. Pure shear on the (1 1 4) plane results in a "pseudo-twin", and interchange shuffles are necessary to convert this to a "reflective" twin and render a lower energy state. Additional atomic shifts at the twin-matrix interfaces result in "sharp" boundaries, further lowering the energy barriers. We established the energy barrier to be 148 mJ m-2 during (114)[221̄] twin boundary growth of four layers at a time. The entire potential energy surface and the mean energy path during twinning can be derived from our simulations, providing the required insight into the atomistic processes involved.

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Energetics of (1 1 4) twinning in B2 NiTi under coupled shear and shuffle. / Ezaz, Tawhid; Sehitoglu, Huseyin; Maier, Hans Jürgen.
in: Acta materialia, Jahrgang 60, Nr. 1, 04.11.2011, S. 339-348.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Ezaz T, Sehitoglu H, Maier HJ. Energetics of (1 1 4) twinning in B2 NiTi under coupled shear and shuffle. Acta materialia. 2011 Nov 4;60(1):339-348. doi: 10.1016/j.actamat.2011.09.032
Ezaz, Tawhid ; Sehitoglu, Huseyin ; Maier, Hans Jürgen. / Energetics of (1 1 4) twinning in B2 NiTi under coupled shear and shuffle. in: Acta materialia. 2011 ; Jahrgang 60, Nr. 1. S. 339-348.
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AU - Maier, Hans Jürgen

N1 - Funding information: The work is supported by the National Science Foundation under DMR-0803270. We acknowledge earlier discussions with Prof. D.D. Johnson on PES. The authors gratefully acknowledge the use of the parallel computing resources part of the Taub cluster provided by the Computational Science and Engineering Program at the University of Illinois, and also partial support from CMMI-1130031.

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N2 - The (1 1 4) twin growth in the austenitic regime in NiTi (B2 lattice) is characterized precisely at the atomistic scale. This twinning mode is consistent with experimental observations but has not been well understood despite its importance. Combined shears, shuffles and interface shifts operate in a complex way to generate the (1 1 4) twin. Pure shear on the (1 1 4) plane results in a "pseudo-twin", and interchange shuffles are necessary to convert this to a "reflective" twin and render a lower energy state. Additional atomic shifts at the twin-matrix interfaces result in "sharp" boundaries, further lowering the energy barriers. We established the energy barrier to be 148 mJ m-2 during (114)[221̄] twin boundary growth of four layers at a time. The entire potential energy surface and the mean energy path during twinning can be derived from our simulations, providing the required insight into the atomistic processes involved.

AB - The (1 1 4) twin growth in the austenitic regime in NiTi (B2 lattice) is characterized precisely at the atomistic scale. This twinning mode is consistent with experimental observations but has not been well understood despite its importance. Combined shears, shuffles and interface shifts operate in a complex way to generate the (1 1 4) twin. Pure shear on the (1 1 4) plane results in a "pseudo-twin", and interchange shuffles are necessary to convert this to a "reflective" twin and render a lower energy state. Additional atomic shifts at the twin-matrix interfaces result in "sharp" boundaries, further lowering the energy barriers. We established the energy barrier to be 148 mJ m-2 during (114)[221̄] twin boundary growth of four layers at a time. The entire potential energy surface and the mean energy path during twinning can be derived from our simulations, providing the required insight into the atomistic processes involved.

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