1989
DOI: 10.1016/0036-9748(89)90054-9
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Unusual strain recovery in γ1′ martensite single variant of CuAlNi alloy

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Cited by 5 publications
(3 citation statements)
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“…Figure c shows the pseudoelastic behavior in cycle 140, which is fully reproducible once the martensite phase becomes completely stabilized and encloses a smaller area in the depth‐load space, indicating that a certain amount of mechanical energy is still dissipated during one loading‐unloading cycle. This mechanical response, named as rubber‐like behavior or pseudoelastic‐twinning, is characteristic of the martensitic state and associated to the hysteretic motion of the martensite interfaces between different variants crystallographically equivalent but with different orientations to minimize the elastic strain energy …”
Section: Resultsmentioning
confidence: 99%
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“…Figure c shows the pseudoelastic behavior in cycle 140, which is fully reproducible once the martensite phase becomes completely stabilized and encloses a smaller area in the depth‐load space, indicating that a certain amount of mechanical energy is still dissipated during one loading‐unloading cycle. This mechanical response, named as rubber‐like behavior or pseudoelastic‐twinning, is characteristic of the martensitic state and associated to the hysteretic motion of the martensite interfaces between different variants crystallographically equivalent but with different orientations to minimize the elastic strain energy …”
Section: Resultsmentioning
confidence: 99%
“…This mechanical response, named as rubber-like behavior or pseudoelastic-twinning, is characteristic of the martensitic state and associated to the hysteretic motion of the martensite interfaces between different variants crystallographically equivalent but with different orientations to minimize the elastic strain energy. [38,39] In order to verify if the stabilized martensite phase can return back to the superelastic behavior, a slight heating of the bulk sample, not exceeding 373 K, was performed, by touching the sample with the tip of a soldering iron, to produce the reverse martensitic transformation. This slight heating is not expected to produce any other microstructural evolution because these samples have an atomic order L2 1 being thermally stable even at 473 K; diffusion processes are only activated above this temperature and dislocations in this L2 1 lattice start moving thermally at 750 K as confirmed by in-situ transmission electron microscopy and internal friction measurements.…”
Section: Anomalous Behavior During Cyclingmentioning
confidence: 99%
“…This variant selection by external stress is at the origin of the transformation strain and superelasticity in shape memory alloys 39 . Otsuka and co-workers 45 48 have succeeded in making and investigating the deformation behaviour of single-crystalline martensite of Cu-Al-Ni SMAs by this method.…”
Section: Introductionmentioning
confidence: 99%