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Page 77

April 16-17, 2018 Las Vegas, Nevada, USA

2

nd

Edition of

Graphene & Semiconductors | Diamond Graphite & Carbon Materials Conference

6

th

Edition of

Smart Materials & Structures Conference

&

Journal of Material Sciences and Engineering| ISSN: 2169-0022 | GDCSM-2018 | Volume: 7

About the order-disorder transition in arc melted Fe

3

SiAlx soft alloys

A Boulouma

1,2

, A. Drici

2

and

A. K. Gangopadhahay

3

1

ESTI of Annaba, Algeria

2

University of Annaba, Algeria

3

Washington University in St Louis, USA

T

here is an increasing interest in soft magnetic Fe-Si-Al alloys due to their promising properties for applications in various

fields; however, all these structural and magnetic properties depend on the structure of the composition alloys The Fe-rich

side of the phase diagram of the Fe-Al, Fe-Si and Fe-Al-Si systems presents the same structures; at room temperature, Fe-Al system

is characterized by a wide range of ferromagnetic disordered body centered cubic solid solution (A2) up to 22 at.% Al at room

temperature. On increasing the Al content, the first intermetallic structure is Fe

3

Al with D0

3

cubic structure and it exists over the 18-

32 at.% Al range. The other stable intermetallic structure is FeAl, which is also cubic with B2 structure (CsCl) and it exists over the

range 32-50 at.% Al. The magnetic behavior of ordered Fe-Al alloys is complex in the 27 to 32 at.% Al region where the magnetization

actually decreases with decreasing temperature. It was found that partial substitution of Al by Si leads to significantly improved D0

3

structural stability against ordered B2 structure and disordered A2 structure. Moreover, there have been extensive studies, both

experimentally and theoretically, of order-disorder transitions of Fe-rich ternary alloys. Mutual solid solubility between Fe

3

Al and

Fe3Si is well-established. The solid solubility and the magnetic behavior of Fe

3

(Al,Si) was correlated with the ratio of electron-atom .

Polishchuk and Katsnel´son studied the existence of the ordered phases

α

1 (Fe

3

Al and Fe

3

Si which have D0

3

or BiF

3

type order) and

α

2

(FeAl and FeSi which have B2 or CsCl type order) along the Fe

3

Al-Fe

3

Si section by means of high temperature X-ray diffraction

and recording the disappearance of D0

3

superlattice (111) and (200) reflections as a function of temperature and composition. In this

work, alloys of nominal compositions of sendust Fe

3

SiAlX (X =1, 0.75, 0.5, 0.25). The phase purities of the arc-melted ingots were

studied by x-ray diffraction using a Rigaku D-MaxB X-ray diffractometer with Cu-K

α

radiation. It was found that decreasing Al

leads to more disorder in the alloy by the formation of

α

-Fe solid solution. However, the addition of Al influences both of the lattice

parameter and crystallite size of the Fe

3

Si phase. Results show that the presence of

α

1

-Al

0.3

Fe

3

Si0.7 with a (422) preferred orientation

has been noticed over the 70 at% Fe range.

bouloumaa@gmail.com

J Material Sci Eng 2018, Volume: 7

DOI: 10.4172/2169-0022-C3-098