NickelMaghrebV1, PascalFrancis, Curation, bibRecord, 000372

New composites of ZnO-P2O5/Ni having PTC transition and high Seebeck coefficient

Identifieur interne : 000372 ( PascalFrancis/Curation ); précédent : 000371; suivant : 000373

New composites of ZnO-P2O5/Ni having PTC transition and high Seebeck coefficient

Auteurs : A. Maaroufi [Maroc] ; O. Oabi [Maroc] ; B. Lucas [France] ; A. El Amrani [Maroc] ; S. Degot [France]

Source :

Journal of non-crystalline solids [ 0022-3093 ] ; 2012.

RBID : Pascal:13-0090410

Descripteurs français

Pascal (Inist)
- Effet Seebeck, Conductivité électrique, Nickel, Fraction volumique, Transition phase, Percolation, Porteur charge, Dépendance température, Coefficient température, Expansion volume, Energie activation, Haute température, Conduction saut, Propriété électrique, Matériau composite, Verre, ZnO, P2O5, 7280N, 8105K, 7220E.
Wicri :
- topic : Nickel, Matériau composite, Verre.

English descriptors

KwdEn :
- Activation energy, Charge carriers, Composite materials, Electrical conductivity, Electrical properties, Glass, High temperature, Hopping conduction, Nickel, Percolation, Phase transitions, Seebeck effect, Temperature coefficient, Temperature dependence, Volume expansion, Volume fraction.

Abstract

In this article, we report the electrical conductivity (σ) and Seebeck coefficient (S) of ZnO-P₂O₅ matrix filled with conductive powder of nickel (Ni). The variation of σ versus volume fraction of Ni showed a non-conducting to conducting phase transition at percolation threshold (28 vol. %). The change of S from high positive to negative values exhibits that this transition is accompanied by the passing of carrier charge from p to n type. On the other hand, the measurements of σ and S as function of temperature, above the percolation threshold, showed a positive temperature coefficient (PTC) phase transition at T_c≥400 K, linked with a high S = -5000 μV/K, giving highest power factor PF=σ.S^2≃2.10^-4 Wm^-1 K^-2. The temperature dependence of the volume expansion enabled to confirm that this transition is associated to the thermal volume variation in matrix. However, the temperature dependence of σ below the percolation threshold showed two different mechanisms: thermally activated hopping behavior at high temperatures and Mott's variable range hopping (VRH) at low temperatures.

A01	`01`	`1`		`@0 0022-3093`
A02	`01`			`@0 JNCSBJ`
A03		`1`		`@0 J. non-cryst. solids`
A05				`@2 358`
A06				`@2 23`
A08	`01`	`1`	`ENG`	`@1 New composites of ZnO-P₂O₅/Ni having PTC transition and high Seebeck coefficient`
A11	`01`	`1`		`@1 MAAROUFI (A.)`
A11	`02`	`1`		`@1 OABI (O.)`
A11	`03`	`1`		`@1 LUCAS (B.)`
A11	`04`	`1`		`@1 EL AMRANI (A.)`
A11	`05`	`1`		`@1 DEGOT (S.)`
A14	`01`			`@1 University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014 @2 Rabat-Agdal @3 MAR @Z 1 aut. @Z 2 aut.`
A14	`02`			`@1 XLIM UMR 6172-Université de Limoges/CNRS 123 avenue Albert Thomas- @2 87060 Limoges @3 FRA @Z 3 aut.`
A14	`03`			`@1 LPSMS, FST Errachidia, University Moulay Ismail Meknès, B. P. 509, Boutalamine @2 , Errachidia @3 MAR @Z 4 aut.`
A14	`04`			`@1 SPCTS, CNRS UMR 6638, European Ceramic Center, 12, rue Atlantis @2 87068 Limoges @3 FRA @Z 5 aut.`
A20				`@1 3312-3317`
A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 14572 @5 354000506890750400`
A44				`@0 0000 @1 © 2013 INIST-CNRS. All rights reserved.`
A45				`@0 46 ref.`
A47	`01`	`1`		`@0 13-0090410`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of non-crystalline solids`
A66	`01`			`@0 GBR`
C01	`01`		`ENG`	@0 In this article, we report the electrical conductivity (σ) and Seebeck coefficient (S) of ZnO-P₂O₅ matrix filled with conductive powder of nickel (Ni). The variation of σ versus volume fraction of Ni showed a non-conducting to conducting phase transition at percolation threshold (28 vol. %). The change of S from high positive to negative values exhibits that this transition is accompanied by the passing of carrier charge from p to n type. On the other hand, the measurements of σ and S as function of temperature, above the percolation threshold, showed a positive temperature coefficient (PTC) phase transition at T_c≥400 K, linked with a high S = -5000 μV/K, giving highest power factor PF=σ.S^2≃2.10^-4 Wm^-1 K^-2. The temperature dependence of the volume expansion enabled to confirm that this transition is associated to the thermal volume variation in matrix. However, the temperature dependence of σ below the percolation threshold showed two different mechanisms: thermally activated hopping behavior at high temperatures and Mott's variable range hopping (VRH) at low temperatures.
C02	`01`	`3`		`@0 001B70B20E`
C02	`02`	`3`		`@0 001B80A05K`
C02	`03`	`3`		`@0 001B70B80N`
C03	`01`	`3`	`FRE`	`@0 Effet Seebeck @5 01`
C03	`01`	`3`	`ENG`	`@0 Seebeck effect @5 01`
C03	`02`	`3`	`FRE`	`@0 Conductivité électrique @5 02`
C03	`02`	`3`	`ENG`	`@0 Electrical conductivity @5 02`
C03	`03`	`3`	`FRE`	`@0 Nickel @2 NC @5 03`
C03	`03`	`3`	`ENG`	`@0 Nickel @2 NC @5 03`
C03	`04`	`X`	`FRE`	`@0 Fraction volumique @5 04`
C03	`04`	`X`	`ENG`	`@0 Volume fraction @5 04`
C03	`04`	`X`	`SPA`	`@0 Fracción volumétrica @5 04`
C03	`05`	`X`	`FRE`	`@0 Transition phase @5 05`
C03	`05`	`X`	`ENG`	`@0 Phase transitions @5 05`
C03	`05`	`X`	`SPA`	`@0 Transición fase @5 05`
C03	`06`	`3`	`FRE`	`@0 Percolation @5 06`
C03	`06`	`3`	`ENG`	`@0 Percolation @5 06`
C03	`07`	`3`	`FRE`	`@0 Porteur charge @5 07`
C03	`07`	`3`	`ENG`	`@0 Charge carriers @5 07`
C03	`08`	`3`	`FRE`	`@0 Dépendance température @5 08`
C03	`08`	`3`	`ENG`	`@0 Temperature dependence @5 08`
C03	`09`	`3`	`FRE`	`@0 Coefficient température @5 09`
C03	`09`	`3`	`ENG`	`@0 Temperature coefficient @5 09`
C03	`10`	`X`	`FRE`	`@0 Expansion volume @5 10`
C03	`10`	`X`	`ENG`	`@0 Volume expansion @5 10`
C03	`10`	`X`	`SPA`	`@0 Expansión volumen @5 10`
C03	`11`	`3`	`FRE`	`@0 Energie activation @5 11`
C03	`11`	`3`	`ENG`	`@0 Activation energy @5 11`
C03	`12`	`X`	`FRE`	`@0 Haute température @5 12`
C03	`12`	`X`	`ENG`	`@0 High temperature @5 12`
C03	`12`	`X`	`SPA`	`@0 Alta temperatura @5 12`
C03	`13`	`3`	`FRE`	`@0 Conduction saut @5 13`
C03	`13`	`3`	`ENG`	`@0 Hopping conduction @5 13`
C03	`14`	`3`	`FRE`	`@0 Propriété électrique @5 14`
C03	`14`	`3`	`ENG`	`@0 Electrical properties @5 14`
C03	`15`	`3`	`FRE`	`@0 Matériau composite @5 15`
C03	`15`	`3`	`ENG`	`@0 Composite materials @5 15`
C03	`16`	`3`	`FRE`	`@0 Verre @5 16`
C03	`16`	`3`	`ENG`	`@0 Glass @5 16`
C03	`17`	`3`	`FRE`	`@0 ZnO @4 INC @5 46`
C03	`18`	`3`	`FRE`	`@0 P2O5 @4 INC @5 47`
C03	`19`	`3`	`FRE`	`@0 7280N @4 INC @5 65`
C03	`20`	`3`	`FRE`	`@0 8105K @4 INC @5 71`
C03	`21`	`3`	`FRE`	`@0 7220E @4 INC @5 72`
N21				`@1 063`

Links toward previous steps (curation, corpus...)

to stream PascalFrancis, to step Corpus: Pour aller vers cette notice dans l'étape Curation :000069

Links to Exploration step

Pascal:13-0090410

Le document en format XML

<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">New composites of ZnO-P<sub>2</sub>
O<sub>5</sub>
/Ni having PTC transition and high Seebeck coefficient</title>
<author><name sortKey="Maaroufi, A" sort="Maaroufi, A" uniqKey="Maaroufi A" first="A." last="Maaroufi">A. Maaroufi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014</s1>
<s2>Rabat-Agdal</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Oabi, O" sort="Oabi, O" uniqKey="Oabi O" first="O." last="Oabi">O. Oabi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014</s1>
<s2>Rabat-Agdal</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Lucas, B" sort="Lucas, B" uniqKey="Lucas B" first="B." last="Lucas">B. Lucas</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>XLIM UMR 6172-Université de Limoges/CNRS 123 avenue Albert Thomas-</s1>
<s2>87060 Limoges</s2>
<s3>FRA</s3>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="El Amrani, A" sort="El Amrani, A" uniqKey="El Amrani A" first="A." last="El Amrani">A. El Amrani</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>LPSMS, FST Errachidia, University Moulay Ismail Meknès, B. P. 509, Boutalamine</s1>
<s2>, Errachidia</s2>
<s3>MAR</s3>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Degot, S" sort="Degot, S" uniqKey="Degot S" first="S." last="Degot">S. Degot</name>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>SPCTS, CNRS UMR 6638, European Ceramic Center, 12, rue Atlantis</s1>
<s2>87068 Limoges</s2>
<s3>FRA</s3>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
</titleStmt>
<publicationStmt><idno type="wicri:source">INIST</idno>
<idno type="inist">13-0090410</idno>
<date when="2012">2012</date>
<idno type="stanalyst">PASCAL 13-0090410 INIST</idno>
<idno type="RBID">Pascal:13-0090410</idno>
<idno type="wicri:Area/PascalFrancis/Corpus">000069</idno>
<idno type="wicri:Area/PascalFrancis/Curation">000372</idno>
</publicationStmt>
<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">New composites of ZnO-P<sub>2</sub>
O<sub>5</sub>
/Ni having PTC transition and high Seebeck coefficient</title>
<author><name sortKey="Maaroufi, A" sort="Maaroufi, A" uniqKey="Maaroufi A" first="A." last="Maaroufi">A. Maaroufi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014</s1>
<s2>Rabat-Agdal</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Oabi, O" sort="Oabi, O" uniqKey="Oabi O" first="O." last="Oabi">O. Oabi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014</s1>
<s2>Rabat-Agdal</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Lucas, B" sort="Lucas, B" uniqKey="Lucas B" first="B." last="Lucas">B. Lucas</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>XLIM UMR 6172-Université de Limoges/CNRS 123 avenue Albert Thomas-</s1>
<s2>87060 Limoges</s2>
<s3>FRA</s3>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="El Amrani, A" sort="El Amrani, A" uniqKey="El Amrani A" first="A." last="El Amrani">A. El Amrani</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>LPSMS, FST Errachidia, University Moulay Ismail Meknès, B. P. 509, Boutalamine</s1>
<s2>, Errachidia</s2>
<s3>MAR</s3>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Degot, S" sort="Degot, S" uniqKey="Degot S" first="S." last="Degot">S. Degot</name>
<affiliation wicri:level="1"><inist:fA14 i1="04"><s1>SPCTS, CNRS UMR 6638, European Ceramic Center, 12, rue Atlantis</s1>
<s2>87068 Limoges</s2>
<s3>FRA</s3>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Journal of non-crystalline solids</title>
<title level="j" type="abbreviated">J. non-cryst. solids</title>
<idno type="ISSN">0022-3093</idno>
<imprint><date when="2012">2012</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Journal of non-crystalline solids</title>
<title level="j" type="abbreviated">J. non-cryst. solids</title>
<idno type="ISSN">0022-3093</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Activation energy</term>
<term>Charge carriers</term>
<term>Composite materials</term>
<term>Electrical conductivity</term>
<term>Electrical properties</term>
<term>Glass</term>
<term>High temperature</term>
<term>Hopping conduction</term>
<term>Nickel</term>
<term>Percolation</term>
<term>Phase transitions</term>
<term>Seebeck effect</term>
<term>Temperature coefficient</term>
<term>Temperature dependence</term>
<term>Volume expansion</term>
<term>Volume fraction</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Effet Seebeck</term>
<term>Conductivité électrique</term>
<term>Nickel</term>
<term>Fraction volumique</term>
<term>Transition phase</term>
<term>Percolation</term>
<term>Porteur charge</term>
<term>Dépendance température</term>
<term>Coefficient température</term>
<term>Expansion volume</term>
<term>Energie activation</term>
<term>Haute température</term>
<term>Conduction saut</term>
<term>Propriété électrique</term>
<term>Matériau composite</term>
<term>Verre</term>
<term>ZnO</term>
<term>P2O5</term>
<term>7280N</term>
<term>8105K</term>
<term>7220E</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Nickel</term>
<term>Matériau composite</term>
<term>Verre</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">In this article, we report the electrical conductivity (σ) and Seebeck coefficient (S) of ZnO-P<sub>2</sub>
O<sub>5</sub>
 matrix filled with conductive powder of nickel (Ni). The variation of σ versus volume fraction of Ni showed a non-conducting to conducting phase transition at percolation threshold (28 vol. %). The change of S from high positive to negative values exhibits that this transition is accompanied by the passing of carrier charge from p to n type. On the other hand, the measurements of σ and S as function of temperature, above the percolation threshold, showed a positive temperature coefficient (PTC) phase transition at T<sub>c</sub>
≥400 K, linked with a high S = -5000 μV/K, giving highest power factor PF=σ.S<sup>2≃</sup>
2.10<sup>-4</sup>
 Wm<sup>-1</sup>
 K<sup>-2</sup>
. The temperature dependence of the volume expansion enabled to confirm that this transition is associated to the thermal volume variation in matrix. However, the temperature dependence of σ below the percolation threshold showed two different mechanisms: thermally activated hopping behavior at high temperatures and Mott's variable range hopping (VRH) at low temperatures.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-3093</s0>
</fA01>
<fA02 i1="01"><s0>JNCSBJ</s0>
</fA02>
<fA03 i2="1"><s0>J. non-cryst. solids</s0>
</fA03>
<fA05><s2>358</s2>
</fA05>
<fA06><s2>23</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>New composites of ZnO-P<sub>2</sub>
O<sub>5</sub>
/Ni having PTC transition and high Seebeck coefficient</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>MAAROUFI (A.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>OABI (O.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>LUCAS (B.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>EL AMRANI (A.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>DEGOT (S.)</s1>
</fA11>
<fA14 i1="01"><s1>University Mohammed VAgdal, Laboratory of Composite Materials, Polymers and Environment, Department of Chemistry, Faculty of Sciences P.B. 1014</s1>
<s2>Rabat-Agdal</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>XLIM UMR 6172-Université de Limoges/CNRS 123 avenue Albert Thomas-</s1>
<s2>87060 Limoges</s2>
<s3>FRA</s3>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>LPSMS, FST Errachidia, University Moulay Ismail Meknès, B. P. 509, Boutalamine</s1>
<s2>, Errachidia</s2>
<s3>MAR</s3>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>SPCTS, CNRS UMR 6638, European Ceramic Center, 12, rue Atlantis</s1>
<s2>87068 Limoges</s2>
<s3>FRA</s3>
<sZ>5 aut.</sZ>
</fA14>
<fA20><s1>3312-3317</s1>
</fA20>
<fA21><s1>2012</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14572</s2>
<s5>354000506890750400</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2013 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>46 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>13-0090410</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Journal of non-crystalline solids</s0>
</fA64>
<fA66 i1="01"><s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>In this article, we report the electrical conductivity (σ) and Seebeck coefficient (S) of ZnO-P<sub>2</sub>
O<sub>5</sub>
 matrix filled with conductive powder of nickel (Ni). The variation of σ versus volume fraction of Ni showed a non-conducting to conducting phase transition at percolation threshold (28 vol. %). The change of S from high positive to negative values exhibits that this transition is accompanied by the passing of carrier charge from p to n type. On the other hand, the measurements of σ and S as function of temperature, above the percolation threshold, showed a positive temperature coefficient (PTC) phase transition at T<sub>c</sub>
≥400 K, linked with a high S = -5000 μV/K, giving highest power factor PF=σ.S<sup>2≃</sup>
2.10<sup>-4</sup>
 Wm<sup>-1</sup>
 K<sup>-2</sup>
. The temperature dependence of the volume expansion enabled to confirm that this transition is associated to the thermal volume variation in matrix. However, the temperature dependence of σ below the percolation threshold showed two different mechanisms: thermally activated hopping behavior at high temperatures and Mott's variable range hopping (VRH) at low temperatures.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70B20E</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B80A05K</s0>
</fC02>
<fC02 i1="03" i2="3"><s0>001B70B80N</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Effet Seebeck</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Seebeck effect</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Conductivité électrique</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Electrical conductivity</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Nickel</s0>
<s2>NC</s2>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Nickel</s0>
<s2>NC</s2>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Fraction volumique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Volume fraction</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Fracción volumétrica</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Transition phase</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Phase transitions</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Transición fase</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Percolation</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Percolation</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Porteur charge</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Charge carriers</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Dépendance température</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Temperature dependence</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Coefficient température</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Temperature coefficient</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Expansion volume</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Volume expansion</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Expansión volumen</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Energie activation</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Activation energy</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Haute température</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>High temperature</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Alta temperatura</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Conduction saut</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Hopping conduction</s0>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Propriété électrique</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Electrical properties</s0>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Matériau composite</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Composite materials</s0>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Verre</s0>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Glass</s0>
<s5>16</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>ZnO</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>P2O5</s0>
<s4>INC</s4>
<s5>47</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>7280N</s0>
<s4>INC</s4>
<s5>65</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>8105K</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>7220E</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03>
<fN21><s1>063</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

Pour manipuler ce document sous Unix (Dilib)

EXPLOR_STEP=$WICRI_ROOT/Wicri/Terre/explor/NickelMaghrebV1/Data/PascalFrancis/Curation

HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 000372 | SxmlIndent | more

HfdSelect -h $EXPLOR_AREA/Data/PascalFrancis/Curation/biblio.hfd -nk 000372 | SxmlIndent | more

Pour mettre un lien sur cette page dans le réseau Wicri

{{Explor lien
   |wiki=    Wicri/Terre
   |area=    NickelMaghrebV1
   |flux=    PascalFrancis
   |étape=   Curation
   |type=    RBID
   |clé=     Pascal:13-0090410
   |texte=   New composites of ZnO-P2O5/Ni having PTC transition and high Seebeck coefficient
}}

This area was generated with Dilib version V0.6.27.
Data generation: Fri Mar 24 23:14:20 2017. Site generation: Tue Mar 5 17:03:47 2024

	Serveur d'exploration sur le nickel au Maghreb
	Attention, ce site est en cours de développement ! Attention, site généré par des moyens informatiques à partir de corpus bruts. Les informations ne sont donc pas validées.

Serveur d'exploration sur le nickel au Maghreb

New composites of ZnO-P2O5/Ni having PTC transition and high Seebeck coefficient

New composites of ZnO-P2O5/Ni having PTC transition and high Seebeck coefficient

Source :

Descripteurs français

English descriptors

Abstract

Links toward previous steps (curation, corpus...)

Links to Exploration step

Le document en format XML

Pour manipuler ce document sous Unix (Dilib)

Pour mettre un lien sur cette page dans le réseau Wicri