1981
DOI: 10.1016/0001-6160(81)90091-2
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The crystallography of the martensitic transformation in equiatomic nickel-titanium

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Cited by 275 publications
(128 citation statements)
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“…The spots derived from the M and the T1 are in mirror symmetry of each other with respect to the (111( ) plane, whereas the spots derived from the M and T2 are consistent with Fig. 2(c) in the work of Knowles and Smith [3], in which the 011 Type II twinning was first reported in the martensite in TiNi alloy. It could be conjectured that no considerable macroscopic strain could be available through variant coalescence, the further deformation procedure would take place mainly inside the martensite variants and the further rearrangement of substructural bands would occur, especially between the 011 Type II and the (111( ) Type I twinning plates.…”
Section: E6olution Of the Cold-drawn Microstructure With Area Reductionsupporting
confidence: 87%
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“…The spots derived from the M and the T1 are in mirror symmetry of each other with respect to the (111( ) plane, whereas the spots derived from the M and T2 are consistent with Fig. 2(c) in the work of Knowles and Smith [3], in which the 011 Type II twinning was first reported in the martensite in TiNi alloy. It could be conjectured that no considerable macroscopic strain could be available through variant coalescence, the further deformation procedure would take place mainly inside the martensite variants and the further rearrangement of substructural bands would occur, especially between the 011 Type II and the (111( ) Type I twinning plates.…”
Section: E6olution Of the Cold-drawn Microstructure With Area Reductionsupporting
confidence: 87%
“…Yet, with the increase of the area reduction, the amount of the 011 Type II twinning gradually reduces. As is well known, the 011 Type II twinning is the most frequently observed twinning mode in the thermal martensite [5], which has also been pointed out theoretically to be a lattice invariant shear [3,4]. Since the microstructure is wholly martensitic at the room temperature for the present alloy before cold-drawing, the appearance of the 011 Type II twinning bands is clearly to provide the necessary lattice invariant shear during the martensitic transformation which had finished before cold-drawing.…”
Section: Discussionsupporting
confidence: 67%
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“…Here, the paper by Knowles and Smith [11] and that by Matsumoto, Miyazaki, Otsuka and Tamura [12], the calculations based on the phenomenological theory, are referred to. The rational interface plane, (1, 1, 0) for ƒ ϭ 0.2710 and (1, 1, Ϫ1) for ƒ ϭ 0.3102, were also reported by both groups.…”
Section: Comparison With Phenomenological Theory Calculationsmentioning
confidence: 99%