NickelMaghrebV1, PascalFrancis, Curation, bibRecord, 000213

X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe50Ni50 alloy prepared by mechanical alloying

Identifieur interne : 000213 ( PascalFrancis/Curation ); précédent : 000212; suivant : 000214

X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe50Ni50 alloy prepared by mechanical alloying

Auteurs : A. Guittoum [Algérie] ; A. Layadi [Algérie] ; A. Bourzami [Algérie] ; H. Tafat [Algérie] ; N. Souami [Algérie] ; S. Boutarfaia [Algérie] ; D. Lacour [France]

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2008.

RBID : Pascal:08-0253702

Descripteurs français

Pascal (Inist)
- Diffraction RX, Microstructure, Effet Mössbauer, Aimantation saturation, Alliage mécanique, Broyeur boulet, Broyeur satellite, Microscopie électronique balayage, Force coercitive, Hystérésis magnétique, Paramètre cristallin, Fer alliage, Nanocristal, Nickel alliage, Métal transition alliage.

English descriptors

KwdEn :
- Ball mill, Coercive force, Iron alloys, Lattice parameters, Magnetic hysteresis, Mechanical alloying, Microstructure, Moessbauer effect, Nanocrystal, Nickel alloys, Planetary mill, Saturation magnetization, Scanning electron microscopy, Transition element alloys, XRD.

Abstract

Nanocrystalline Fe₅₀Ni₅₀ alloy samples were prepared by the mechanical alloying process using planetary high-energy ball mill. The alloy formation and different physical properties were investigated as a function of milling time, t, (in the 0-50 h range) by means of the X-ray diffraction (XRD) technique, scanning electron microscopy (SEM), energy dispersive X-ray (EDAX), Mössbauer spectroscopy and the vibrating sample magnetometer (VSM). The complete formation of γ-FeNi is observed after 24 h milling. When milling time increases from 0 to 50 h, the lattice parameter increases towards the Fe₅₀Ni₅₀ bulk value, the grain size decreases from 67 to 13 nm, while the strain increases from 0.09% to 0.41%. Grain morphologies at different formation stages were observed by SEM. Saturation magnetization and coercive fields derived from the hysteresis curves are discussed as a function of milling time.

A01	`01`	`1`		`@0 0304-8853`
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A08	`01`	`1`	`ENG`	`@1 X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe₅₀Ni₅₀ alloy prepared by mechanical alloying`
A11	`01`	`1`		`@1 GUITTOUM (A.)`
A11	`02`	`1`		`@1 LAYADI (A.)`
A11	`03`	`1`		`@1 BOURZAMI (A.)`
A11	`04`	`1`		`@1 TAFAT (H.)`
A11	`05`	`1`		`@1 SOUAMI (N.)`
A11	`06`	`1`		`@1 BOUTARFAIA (S.)`
A11	`07`	`1`		`@1 LACOUR (D.)`
A14	`01`			`@1 Nuclear Research Center of Algiers, 2 Bd Frantz Fanon, BP 399, Alger-Gare @2 Alger @3 DZA @Z 1 aut. @Z 5 aut.`
A14	`02`			`@1 Département de Physique, Faculté des Sciences, Université de Sétif @2 19000 @3 DZA @Z 2 aut. @Z 3 aut.`
A14	`03`			`@1 Laboratory S.G.M., UST.H.B., BP 32 @2 Bab-Ezzouar @3 DZA @Z 4 aut.`
A14	`04`			`@1 Centre de Recherche Nucléaire de Draria, BP 43 @2 Alger @3 DZA @Z 6 aut.`
A14	`05`			`@1 LPM, Nancy-University, CNRS @2 54506 Vandoeuvre les Nancy @3 FRA @Z 7 aut.`
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A21				`@1 2008`
A23	`01`			`@0 ENG`
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A44				`@0 0000 @1 © 2008 INIST-CNRS. All rights reserved.`
A45				`@0 37 ref.`
A47	`01`	`1`		`@0 08-0253702`
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A64	`01`	`1`		`@0 Journal of magnetism and magnetic materials`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 Nanocrystalline Fe₅₀Ni₅₀ alloy samples were prepared by the mechanical alloying process using planetary high-energy ball mill. The alloy formation and different physical properties were investigated as a function of milling time, t, (in the 0-50 h range) by means of the X-ray diffraction (XRD) technique, scanning electron microscopy (SEM), energy dispersive X-ray (EDAX), Mössbauer spectroscopy and the vibrating sample magnetometer (VSM). The complete formation of γ-FeNi is observed after 24 h milling. When milling time increases from 0 to 50 h, the lattice parameter increases towards the Fe₅₀Ni₅₀ bulk value, the grain size decreases from 67 to 13 nm, while the strain increases from 0.09% to 0.41%. Grain morphologies at different formation stages were observed by SEM. Saturation magnetization and coercive fields derived from the hysteresis curves are discussed as a function of milling time.
C02	`01`	`3`		`@0 001B80A07B`
C02	`02`	`3`		`@0 001B70F80`
C02	`03`	`3`		`@0 001B70E75`
C03	`01`	`3`	`FRE`	`@0 Diffraction RX @5 02`
C03	`01`	`3`	`ENG`	`@0 XRD @5 02`
C03	`02`	`3`	`FRE`	`@0 Microstructure @5 03`
C03	`02`	`3`	`ENG`	`@0 Microstructure @5 03`
C03	`03`	`3`	`FRE`	`@0 Effet Mössbauer @5 04`
C03	`03`	`3`	`ENG`	`@0 Moessbauer effect @5 04`
C03	`04`	`X`	`FRE`	`@0 Aimantation saturation @5 05`
C03	`04`	`X`	`ENG`	`@0 Saturation magnetization @5 05`
C03	`04`	`X`	`SPA`	`@0 Imanación saturación @5 05`
C03	`05`	`3`	`FRE`	`@0 Alliage mécanique @5 06`
C03	`05`	`3`	`ENG`	`@0 Mechanical alloying @5 06`
C03	`06`	`X`	`FRE`	`@0 Broyeur boulet @5 07`
C03	`06`	`X`	`ENG`	`@0 Ball mill @5 07`
C03	`06`	`X`	`SPA`	`@0 Molino bolas @5 07`
C03	`07`	`X`	`FRE`	`@0 Broyeur satellite @5 08`
C03	`07`	`X`	`ENG`	`@0 Planetary mill @5 08`
C03	`07`	`X`	`SPA`	`@0 Molino rodillos satelite @5 08`
C03	`08`	`3`	`FRE`	`@0 Microscopie électronique balayage @5 09`
C03	`08`	`3`	`ENG`	`@0 Scanning electron microscopy @5 09`
C03	`09`	`3`	`FRE`	`@0 Force coercitive @5 10`
C03	`09`	`3`	`ENG`	`@0 Coercive force @5 10`
C03	`10`	`3`	`FRE`	`@0 Hystérésis magnétique @5 11`
C03	`10`	`3`	`ENG`	`@0 Magnetic hysteresis @5 11`
C03	`11`	`3`	`FRE`	`@0 Paramètre cristallin @5 12`
C03	`11`	`3`	`ENG`	`@0 Lattice parameters @5 12`
C03	`12`	`3`	`FRE`	`@0 Fer alliage @5 15`
C03	`12`	`3`	`ENG`	`@0 Iron alloys @5 15`
C03	`13`	`X`	`FRE`	`@0 Nanocristal @5 16`
C03	`13`	`X`	`ENG`	`@0 Nanocrystal @5 16`
C03	`13`	`X`	`SPA`	`@0 Nanocristal @5 16`
C03	`14`	`3`	`FRE`	`@0 Nickel alliage @5 17`
C03	`14`	`3`	`ENG`	`@0 Nickel alloys @5 17`
C03	`15`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C03	`15`	`3`	`ENG`	`@0 Transition element alloys @5 48`
N21				`@1 162`

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Pascal:08-0253702

Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe<sub>50</sub>
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<term>Mechanical alloying</term>
<term>Microstructure</term>
<term>Moessbauer effect</term>
<term>Nanocrystal</term>
<term>Nickel alloys</term>
<term>Planetary mill</term>
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<term>Broyeur boulet</term>
<term>Broyeur satellite</term>
<term>Microscopie électronique balayage</term>
<term>Force coercitive</term>
<term>Hystérésis magnétique</term>
<term>Paramètre cristallin</term>
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<front><div type="abstract" xml:lang="en">Nanocrystalline Fe<sub>50</sub>
Ni<sub>50</sub>
 alloy samples were prepared by the mechanical alloying process using planetary high-energy ball mill. The alloy formation and different physical properties were investigated as a function of milling time, t, (in the 0-50 h range) by means of the X-ray diffraction (XRD) technique, scanning electron microscopy (SEM), energy dispersive X-ray (EDAX), Mössbauer spectroscopy and the vibrating sample magnetometer (VSM). The complete formation of γ-FeNi is observed after 24 h milling. When milling time increases from 0 to 50 h, the lattice parameter increases towards the Fe<sub>50</sub>
Ni<sub>50</sub>
 bulk value, the grain size decreases from 67 to 13 nm, while the strain increases from 0.09% to 0.41%. Grain morphologies at different formation stages were observed by SEM. Saturation magnetization and coercive fields derived from the hysteresis curves are discussed as a function of milling time.</div>
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 alloy prepared by mechanical alloying</s1>
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<fA14 i1="01"><s1>Nuclear Research Center of Algiers, 2 Bd Frantz Fanon, BP 399, Alger-Gare</s1>
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<s3>DZA</s3>
<sZ>1 aut.</sZ>
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<fA14 i1="02"><s1>Département de Physique, Faculté des Sciences, Université de Sétif</s1>
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<s3>DZA</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="05"><s1>LPM, Nancy-University, CNRS</s1>
<s2>54506 Vandoeuvre les Nancy</s2>
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<fC01 i1="01" l="ENG"><s0>Nanocrystalline Fe<sub>50</sub>
Ni<sub>50</sub>
 alloy samples were prepared by the mechanical alloying process using planetary high-energy ball mill. The alloy formation and different physical properties were investigated as a function of milling time, t, (in the 0-50 h range) by means of the X-ray diffraction (XRD) technique, scanning electron microscopy (SEM), energy dispersive X-ray (EDAX), Mössbauer spectroscopy and the vibrating sample magnetometer (VSM). The complete formation of γ-FeNi is observed after 24 h milling. When milling time increases from 0 to 50 h, the lattice parameter increases towards the Fe<sub>50</sub>
Ni<sub>50</sub>
 bulk value, the grain size decreases from 67 to 13 nm, while the strain increases from 0.09% to 0.41%. Grain morphologies at different formation stages were observed by SEM. Saturation magnetization and coercive fields derived from the hysteresis curves are discussed as a function of milling time.</s0>
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<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Microstructure</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Effet Mössbauer</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Moessbauer effect</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Aimantation saturation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Saturation magnetization</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Imanación saturación</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Alliage mécanique</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Mechanical alloying</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Broyeur boulet</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Ball mill</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Molino bolas</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Broyeur satellite</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Planetary mill</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Molino rodillos satelite</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Microscopie électronique balayage</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Scanning electron microscopy</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Force coercitive</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Coercive force</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Hystérésis magnétique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Magnetic hysteresis</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Paramètre cristallin</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Lattice parameters</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Fer alliage</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Iron alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Nanocristal</s0>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Nanocrystal</s0>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Nanocristal</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Nickel alliage</s0>
<s5>17</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Nickel alloys</s0>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>48</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>48</s5>
</fC03>
<fN21><s1>162</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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	Serveur d'exploration sur le nickel au Maghreb
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Serveur d'exploration sur le nickel au Maghreb

X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe50Ni50 alloy prepared by mechanical alloying

X-ray diffraction, microstructure, Mössbauer and magnetization studies of nanostructured Fe50Ni50 alloy prepared by mechanical alloying

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