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Page 48

April 15-16, 2019 | Frankfurt, Germany

Applied Physics & Laser, Optics and Photonics

International Conference on

Materials Science and Nanotechnology | Volume: 3

Physical basis of shape memory effect and reversibility in shape memory alloys

Osman Adiguzel

Firat University, Turkey

A

series of alloy system take place in a class of

smart materials due to stimulus response to

external effect. Shape memory alloys take place

in this class by exhibiting a peculiar property

called shape memory effect. This phenomenon is

characterized by the recoverability of two certain

shapes of material at different temperatures.

Shape memory materials are used as shape

memory devices in many interdisciplinary fields

such as medicine, metallurgy, building industry

and many engineering fields. Shape memory

effect is performed thermally by heating and

cooling after first cooling and stressing treatments.

Shape memory effect is result of successive

crystallographic transformations; thermal and

stress induced martensitic transformations.

Shape memory alloys exhibit another property

called superelasticity, which is performed by

stressing material at high temperature parent

phase region. This effect exhibit classical elastic

material behavior and it is performed by stressing

and releasing the material in parent phase region.

Loading and unloading paths are different in

stress strain diagram, and cycling loop reveals

energy dissipation. The strain energy is stored

after releasing, and these alloys are mainly used

as deformation absorbent materials in control of

civil structures subjected to seismic events, due

to the absorbance of strain energy during any

disaster or earthquake.

Thermal inducedmartensitic transformation is first

order lattice-distorting phase transformations,

and thermally occurs on cooling, by which ordered

parent phase structures turn into twinned

martensitic structures. This transformation occurs

with cooperative movements of atoms by means

of lattice invariant shear. Lattice invariant shears

occur in two opposite directions, <110 > -type

directions on the {110} - type planes of austenite

matrix which is basal plane of martensite.

Thermal induced martensite occurs as twinned

martensite, and the twinned structures turn into

the detwinned structures by means of stress

induced martensitic transformation by stressing

the material in the martensitic condition.

Copper based alloys exhibit this property in

metastable β-phase region, which has bcc-based

structures at high temperature parent phase field.

Lattice invariant shear and twinning is not uniform

in copper based ternary alloys and gives rise to the

formation of complex layered structures, depending

on the stacking sequences on the close-packed

planes of the ordered parent phase lattice, like 3R,

9R or 18R depending on the stacking sequences

on the close-packed planes of the ordered lattice.

Crystal structure of martensite of these alloys is

orthorhombic and basal plane is hexagonal.

In the present contribution, x-ray diffraction

and transmission electron microscopy (TEM)

studies were carried out on two copper based

CuAlMn and CuZnAl alloys. X-ray diffraction

profiles and electron diffraction patterns reveal

that both alloys exhibit super lattice reflections

inherited from parent phase due to the displacive

character of martensitic transformation. X-ray

diffractograms taken in a long time interval

show that diffraction angles and intensities of

diffraction peaks change with the aging duration

at room temperature. In particular, some of the

successive peak pairs providing a special relation

between Miller indices come close each other.

This result refers to the rearrangement of atoms

in diffusive manner.

e

:

oadiguzel@firat.edu.tr