Cover Picture: Directional Atomic Rearrangements During Transformations Between the α‐ and γ‐Phases in Titanium Aluminides (Adv. Eng. Mater. 4/2008)
Identifieur interne : 002D45 ( Istex/Corpus ); précédent : 002D44; suivant : 002D46Cover Picture: Directional Atomic Rearrangements During Transformations Between the α‐ and γ‐Phases in Titanium Aluminides (Adv. Eng. Mater. 4/2008)
Auteurs : K. Liss ; A. Stark ; A. Bartels ; H. Clemens ; T. Buslaps ; D. Phelan ; L. YeohSource :
- Advanced Engineering Materials [ 1438-1656 ] ; 2008-04.
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Abstract
Making movies in‐situ at glowing temperatures up to 1300 °C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α2‐rich γ‐based TiAl first approaches its equilibrium by α2 → γ on a heating ramp, disorders α2 → α and then evolves reversely γ → α, which are morphologically different processes. More details can be found in the article by K.‐D. Liss et al. on page 389.
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DOI: 10.1002/adem.200890009
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ISTEX:F14BAB7B836481F444C1463F1CC86A8D731EBE48Le document en format XML
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A quenched, α</:t><:t>‐rich γ‐based TiAl first approaches its equilibrium by α</:t><:t>→ γ on a heating ramp, disorders α</:t><:t>→ α and then evolves reversely γ → α, which are morphologically different processes. More details can be found in the article by K.‐D. Liss et al. on page 389.</:t></p></abstract><abstract xml:lang="en" style="graphical"><p><hi rend="subscript">2</hi><hi rend="subscript">2</hi><hi rend="subscript">2</hi><figure type="box"><media mimeType="image" url="urn:x-wiley:14381656:media:ADEM200890009:content"></media><media mimeType="image/gif" rendition="webLoRes"></media><media mimeType="image/gif" rendition="webOriginal"></media><media mimeType="image/gif" rendition="webHiRes"></media></figure><:t>Making movies in‐situ at glowing temperatures up to 1300°C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α</:t><:t>‐rich γ‐based TiAl first approaches its equilibrium by α</:t><:t>→ γ on a heating ramp, disorders α</:t><:t>→ α and then evolves reversely γ → α, which are morphologically different processes.</:t></p></abstract><textClass><keywords xml:lang="en"><term xml:id="kwd1">In‐situ microscopy</term><term xml:id="kwd2">Phase transformations</term><term xml:id="kwd3">Synchrotron radiation</term></keywords><keywords rend="articleCategory"><term>Cover Picture</term></keywords><keywords rend="tocHeading1"><term>Cover Picture</term></keywords></textClass><langUsage><language ident="en"></language></langUsage></profileDesc><revisionDesc><change>undefined</change><change>[object Object]</change></revisionDesc></teiHeader></istex:fulltextTEI><json:item><extension>txt</extension><original>false</original><mimetype>text/plain</mimetype><uri>https://api.istex.fr/document/F14BAB7B836481F444C1463F1CC86A8D731EBE48/fulltext/txt</uri></json:item></fulltext><metadata><istex:metadataXml wicri:clean="Wiley component found"><istex:xmlDeclaration>version="1.0" encoding="UTF-8" standalone="yes"</istex:xmlDeclaration><istex:document><component version="2.0" type="serialArticle" xml:lang="en"><header><publicationMeta level="product"><publisherInfo><publisherName>WILEY‐VCH Verlag</publisherName><publisherLoc>Weinheim</publisherLoc></publisherInfo><doi registered="yes">10.1002/(ISSN)1527-2648</doi><issn type="print">1438-1656</issn><issn type="electronic">1527-2648</issn><idGroup><id type="product" value="ADEM"></id></idGroup><titleGroup><title type="main" xml:lang="en" sort="ADVANCED ENGINEERING MATERIALS">Advanced Engineering Materials</title><title type="short">Adv. 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Mater. 4/2008)</title></titleGroup><creators><creator xml:id="au1" creatorRole="author" affiliationRef="#a1"><personName><givenNames>K.‐D.</givenNames><familyName>Liss</familyName></personName><contactDetails><email>kdl@ansto.gov.au</email><email>liss@kd.liss.de</email></contactDetails></creator><creator xml:id="au2" creatorRole="author" affiliationRef="#a2"><personName><givenNames>A.</givenNames><familyName>Stark</familyName></personName></creator><creator xml:id="au3" creatorRole="author" affiliationRef="#a2"><personName><givenNames>A.</givenNames><familyName>Bartels</familyName></personName></creator><creator xml:id="au4" creatorRole="author" affiliationRef="#a3"><personName><givenNames>H.</givenNames><familyName>Clemens</familyName></personName></creator><creator xml:id="au5" creatorRole="author" affiliationRef="#a4"><personName><givenNames>T.</givenNames><familyName>Buslaps</familyName></personName></creator><creator xml:id="au6" creatorRole="author" affiliationRef="#a5"><personName><givenNames>D.</givenNames><familyName>Phelan</familyName></personName></creator><creator xml:id="au7" creatorRole="author" affiliationRef="#a1"><personName><givenNames>L. A.</givenNames><familyName>Yeoh</familyName></personName></creator></creators><affiliationGroup><affiliation xml:id="a1" countryCode="AU" type="organization"><unparsedAffiliation>The Bragg Institute, Australian Nuclear Science and Technology Organisation, Private Mail Bag 1, Menai NSW 2234 (Australia)</unparsedAffiliation></affiliation><affiliation xml:id="a2" countryCode="DE" type="organization"><unparsedAffiliation>Institute of Materials Science and Technology, Hamburg University of Technology, Eissendorferstrasse 40, D‐21073 Hamburg (Germany)</unparsedAffiliation></affiliation><affiliation xml:id="a3" countryCode="AT" type="organization"><unparsedAffiliation>Department of Physical Metallurgy and Materials Testing, Montanuniversität, Franz‐Josef‐Strasse 18, A‐8700 Leoben (Austria)</unparsedAffiliation></affiliation><affiliation xml:id="a4" countryCode="FR" type="organization"><unparsedAffiliation>European Synchrotron Radiation Facility B. P. 220, F‐38043 Grenoble Cedex (France)</unparsedAffiliation></affiliation><affiliation xml:id="a5" countryCode="AU" type="organization"><unparsedAffiliation>Engineering Materials Institute / Faculty of Engineering, University of Wollongong, Northfield Avenue, Wollongong NSW 2500 (Australia)</unparsedAffiliation></affiliation></affiliationGroup><keywordGroup xml:lang="en" type="author"><keyword xml:id="kwd1">In‐situ microscopy</keyword><keyword xml:id="kwd2">Phase transformations</keyword><keyword xml:id="kwd3">Synchrotron radiation</keyword></keywordGroup><abstractGroup><abstract type="main" xml:lang="fr"><title type="main">Abstract</title><p>Making movies in‐situ at glowing temperatures up to 1300 °C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α<sub>2</sub>‐rich γ‐based TiAl first approaches its equilibrium by α<sub>2</sub> → γ on a heating ramp, disorders α<sub>2</sub> → α and then evolves reversely γ → α, which are morphologically different processes. More details can be found in the article by K.‐D. Liss et al. on page 389.</p></abstract><abstract type="graphical" xml:lang="en"><p>Making movies in‐situ at glowing temperatures up to 1300°C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α<sub>2</sub>‐rich γ‐based TiAl first approaches its equilibrium by α<sub>2</sub> → γ on a heating ramp, disorders α<sub>2</sub> → α and then evolves reversely γ → α, which are morphologically different processes. <blockFixed type="graphic"><mediaResourceGroup><mediaResource alt="image" eRights="yes" copyright="WILEY-VCH" href="urn:x-wiley:14381656:media:ADEM200890009:content"></mediaResource><mediaResource alt="thumbnail image" rendition="webLoRes" mimeType="image/gif" href=""></mediaResource><mediaResource alt="original image" rendition="webOriginal" mimeType="image/gif" href=""></mediaResource><mediaResource alt="magnified image" rendition="webHiRes" mimeType="image/gif" href=""></mediaResource></mediaResourceGroup></blockFixed></p></abstract></abstractGroup></contentMeta></header></component></istex:document></istex:metadataXml><mods version="3.6"><titleInfo lang="en"><title>Cover Picture: Directional Atomic Rearrangements During Transformations Between the α‐ and γ‐Phases in Titanium Aluminides (Adv. Eng. Mater. 4/2008)</title></titleInfo><titleInfo type="alternative" contentType="CDATA" lang="en"><title>Cover Picture: Directional Atomic Rearrangements During Transformations Between the α‐ and γ‐Phases in Titanium Aluminides (Adv. Eng. Mater. 4/2008)</title></titleInfo><name type="personal"><namePart type="given">K.‐D.</namePart><namePart type="family">Liss</namePart><affiliation>E-mail: kdl@ansto.gov.au</affiliation><affiliation>E-mail: liss@kd.liss.de</affiliation><affiliation>The Bragg Institute, Australian Nuclear Science and Technology Organisation, Private Mail Bag 1, Menai NSW 2234 (Australia)</affiliation><affiliation>E-mail: kdl@ansto.gov.au</affiliation><affiliation>E-mail: liss@kd.liss.de</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">A.</namePart><namePart type="family">Stark</namePart><affiliation>Institute of Materials Science and Technology, Hamburg University of Technology, Eissendorferstrasse 40, D‐21073 Hamburg (Germany)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">A.</namePart><namePart type="family">Bartels</namePart><affiliation>Institute of Materials Science and Technology, Hamburg University of Technology, Eissendorferstrasse 40, D‐21073 Hamburg (Germany)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">H.</namePart><namePart type="family">Clemens</namePart><affiliation>Department of Physical Metallurgy and Materials Testing, Montanuniversität, Franz‐Josef‐Strasse 18, A‐8700 Leoben (Austria)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">T.</namePart><namePart type="family">Buslaps</namePart><affiliation>European Synchrotron Radiation Facility B. P. 220, F‐38043 Grenoble Cedex (France)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">D.</namePart><namePart type="family">Phelan</namePart><affiliation>Engineering Materials Institute / Faculty of Engineering, University of Wollongong, Northfield Avenue, Wollongong NSW 2500 (Australia)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">L. A.</namePart><namePart type="family">Yeoh</namePart><affiliation>The Bragg Institute, Australian Nuclear Science and Technology Organisation, Private Mail Bag 1, Menai NSW 2234 (Australia)</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="article" displayLabel="article" authority="ISTEX" authorityURI="https://content-type.data.istex.fr" valueURI="https://content-type.data.istex.fr/ark:/67375/XTP-6N5SZHKN-D">article</genre><originInfo><publisher>WILEY‐VCH Verlag</publisher><place><placeTerm type="text">Weinheim</placeTerm></place><dateIssued encoding="w3cdtf">2008-04</dateIssued><copyrightDate encoding="w3cdtf">2008</copyrightDate></originInfo><language><languageTerm type="code" authority="rfc3066">en</languageTerm><languageTerm type="code" authority="iso639-2b">eng</languageTerm></language><physicalDescription><extent unit="figures">0</extent><extent unit="tables">0</extent><extent unit="references">0</extent></physicalDescription><abstract lang="fr">Making movies in‐situ at glowing temperatures up to 1300 °C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α2‐rich γ‐based TiAl first approaches its equilibrium by α2 → γ on a heating ramp, disorders α2 → α and then evolves reversely γ → α, which are morphologically different processes. More details can be found in the article by K.‐D. Liss et al. on page 389.</abstract><abstract type="graphical" lang="en">Making movies in‐situ at glowing temperatures up to 1300°C through a microscope (false color image) and from two‐dimensional X‐ray diffraction (movie frames) reveal the lattice correlations, gradients and intermediate structures during phase transformations in titanium aluminide. A quenched, α2‐rich γ‐based TiAl first approaches its equilibrium by α2 → γ on a heating ramp, disorders α2 → α and then evolves reversely γ → α, which are morphologically different processes.</abstract><subject lang="en"><genre>keywords</genre><topic>In‐situ microscopy</topic><topic>Phase transformations</topic><topic>Synchrotron radiation</topic></subject><relatedItem type="host"><titleInfo><title>Advanced Engineering Materials</title></titleInfo><titleInfo type="abbreviated"><title>Adv. Eng. 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