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Crystallographic Basis and Mechanism of Shape Reversibility in Shape Memory Alloys
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Journal of Material Sciences & Engineering

ISSN: 2169-0022

Open Access

Commentary - (2022) Volume 11, Issue 1

Crystallographic Basis and Mechanism of Shape Reversibility in Shape Memory Alloys

Osman Adiguzel*
*Correspondence: Osman Adiguzel, Department of Physics, Firat University, Turkey, Email:
Department of Physics, Firat University, Turkey

Received: 01-Feb-2022, Manuscript No. jme-21-50858 ; Editor assigned: 04-Feb-2022, Pre QC No. jme-21-50858 (PQ) ; Reviewed: 18-Feb-2022, QC No. jme-21-50858; Revised: 23-Feb-2022, Manuscript No. jme-21-50858 (R) ; Published: 28-Feb-2022 , DOI: 10.37421/jme.2022.11.04
Citation: Vladimir, Datsko. "The Scope of Surface Electromagnetic Waves (Sew)." J Material Sci Eng 11 (2022); 01
Copyright: © 2022 Osman A. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

Commentary

A series of alloy systems take place in class of advanced smart materials with adaptive properties and stimulus response to the external changes. Shape memory alloys take place in this group, due to the shape reversibility and capacity of responding to changes in the environment. These alloys exhibit a peculiar property called shape memory effect, which is characterized by the recoverability of two certain shapes at different temperatures.

This phenomenon is initiated by cooling and deformation processes and performed thermally on heating and cooling. Therefore this behavior can be called thermoelasticity. These alloys have dual characteristics called thermoelasticity and superelasticity, from viewpoint of memory behavior. Two successive structural transformations, thermal and stress induced martensitic transformations govern shape memory phenomena in crystallographic basis. Thermal induced transformation occurs along with crystal twinning on cooling and ordered parent phase structures turn into twinned martensite structures, and twinned structures turn into the detwinned structures by stressing material in low temperature condition by means of stress induced transformation. Superelasticity is performed mechanically by stressing and releasing material at a constant temperature in parent phase region, and shape recovery is performed simultaneously upon releasing the applied stress. Superelasticity is performed in non-linear way; stressing and releasing paths are different in the stress strain diagram, and hysteresis loop refers to energy dissipation.

The elementary processes involved in such martensitic transformations are lattice invariant shear, lattice twinning and detwinning. It is well known that crystal twinning and detwinning reactions play a considerable role in shape memory effect and superelasticity. Thermal induced martensitic transformation is lattice distorting phase transformation occur with the cooperative movement of atoms by means of shear like mechanism in <110>-type directions on {110}-type planes of austenite matrix.

Copper based ternary alloys exhibit shape memory in β-phase field. Lattice invariant shear and twinning is not uniform in these alloys, and cause to the formation of long period layered martensitic structures with lattice twinning on cooling.

In the present contribution, electron diffraction and x-ray diffraction studies performed on two copper based CuZnAl and CuAlMn alloys. Electron diffraction patterns and x-ray diffraction profiles exhibit super lattice reflection. Specimens of these alloys aged at room temperature, and a series of x-ray diffractions were taken duration aging. Reached results show that diffraction angles and peak intensities change with aging time. Especially, some of the successive peak pairs providing a special relation between Miller indices come close each other, and this result refers to the rearrangement of atoms in diffusive manner.

The major advantages of the CuAlNi system are its wide range of useful transformation temperatures, its stability at elevated temperature making it the only system that can be used for applications above 100°C, its small hysteresis and its relatively low cost.

A new alloy, where the nickel is replaced by beryllium, has recently achieved commercial acceptance. Cu12Al doped with less than 0.5% of beryllium extends the transformation temperature range from 100°C to -200°C. This CuAlBe alloy exhibits excellent superelastic and damping properties.

Acknowledgment

None

Conflict of Interest

Author declares there is no conflict of interest.

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