In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system
Solutal melting was investigated in-situ by means of high temperature laser scanning confocal microscopy. This technique enabled us to track the motion of the solid–liquid interface in order to determine the evolution of the interfacial velocity. The Cu–Ni binary system was chosen as a model case an...
Gespeichert in:
Veröffentlicht in: | Materials characterization 2014-11, Vol.97, p.125-131 |
---|---|
Hauptverfasser: | , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 131 |
---|---|
container_issue | |
container_start_page | 125 |
container_title | Materials characterization |
container_volume | 97 |
creator | Deillon, L. Zollinger, J. Daloz, D. Založnik, M. Combeau, H. |
description | Solutal melting was investigated in-situ by means of high temperature laser scanning confocal microscopy. This technique enabled us to track the motion of the solid–liquid interface in order to determine the evolution of the interfacial velocity. The Cu–Ni binary system was chosen as a model case and concentric samples were fabricated from both pure metals. Two holding temperatures above the melting point of Cu were investigated, i.e., 1115 and 1145°C. As the average composition of the mounted samples was chosen to lie within the solid solution region, the reaction occurred via the following steps: i) thermal melting of Cu, ii) solutal melting of Ni, and iii) resolidification. A smooth and regular s–l interface was observed during solutal melting, except during a short period at 1145°C where an irregularity briefly appeared. At 1115°C, the dissolution of Ni was completed in less than 3min and the total thickness dissolved was in the range 40–50μm. At 1145°C, the dissolution did not last much longer but the total thickness dissolved was significantly larger: approximately 180μm. At both temperatures, the velocity first increased, then reached a maximum value after 20–30s (0.6–0.8μm/s at 1115°C and 4.8μm/s at 1145°C), and finally tends progressively to zero. Post-mortem observations showed that the Ni was homogeneously dissolved over the entire sample height at 1115°C, which excludes any effects of convection on the velocities that we measured. On the contrary, at 1145°C, the dissolution was more important in the upper part of the sample and the interface appeared curved. The total thickness dissolved was in both cases larger than the predicted theoretical values and the melting velocities were also larger than the values obtained from finite difference calculations. The discrepancies are more pronounced at higher temperature.
•Solutal melting was investigated in-situ using laser scanning confocal microscopy.•The kinetics of the process in the Cu/Ni system was determined at 1115 and 1145°C.•A smooth and regular solid–liquid interface was observed.•The dissolution of Ni was completed in less than 3min at both temperatures.•The velocity increased, reached a maximum after 20–30s, and finally tends to zero. |
doi_str_mv | 10.1016/j.matchar.2014.09.004 |
format | Article |
fullrecord | <record><control><sourceid>proquest_hal_p</sourceid><recordid>TN_cdi_hal_primary_oai_HAL_hal_01291907v1</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S1044580314002794</els_id><sourcerecordid>1660039922</sourcerecordid><originalsourceid>FETCH-LOGICAL-c406t-9b46f600bc80b787d3ef681293274279e7a2d801cb81cbd0c5ef712e8a51c1a73</originalsourceid><addsrcrecordid>eNqFkU2L2zAQhk1podttf0JBl0J7sHckO5bUS1lC210I7WV7FrI8bhRkKZXkQP79yiTstQJ98sw7o3mr6iOFhgLt7w7NrLPZ69gwoF0DsgHoXlU3VPC27qiQr8sZuq7eCGjfVu9SOgBALyi_qfaPvk42LyQMCeNJZxt8ImEiKbgla0dmdNn6v2RJ6-p0oUgy2vv1aoKfglkpa2JIJhzPX8nTHsl2uftlyRxGdCSdU8b5ffVm0i7hh-t-W_358f1p-1Dvfv983N7vatNBn2s5dP3UAwxGwMAFH1ucSqVMtox3jEvkmo0CqBlEmSOYDU6cMhR6Qw3VvL2tvlx099qpY7SzjmcVtFUP9zu1vkERoxL4iRb284U9xvBvwZTVbJNB57THsCRF-1JJKyVjBd1c0PWfKeL0ok1BrS6og7q6oFYXFEhVXChxn64pdOmam6L2xqaXYCbKAL7qf7twWHpzshhVMha9wdFGNFmNwf4n0zNFwqAX</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1660039922</pqid></control><display><type>article</type><title>In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system</title><source>Elsevier ScienceDirect Journals</source><creator>Deillon, L. ; Zollinger, J. ; Daloz, D. ; Založnik, M. ; Combeau, H.</creator><creatorcontrib>Deillon, L. ; Zollinger, J. ; Daloz, D. ; Založnik, M. ; Combeau, H.</creatorcontrib><description>Solutal melting was investigated in-situ by means of high temperature laser scanning confocal microscopy. This technique enabled us to track the motion of the solid–liquid interface in order to determine the evolution of the interfacial velocity. The Cu–Ni binary system was chosen as a model case and concentric samples were fabricated from both pure metals. Two holding temperatures above the melting point of Cu were investigated, i.e., 1115 and 1145°C. As the average composition of the mounted samples was chosen to lie within the solid solution region, the reaction occurred via the following steps: i) thermal melting of Cu, ii) solutal melting of Ni, and iii) resolidification. A smooth and regular s–l interface was observed during solutal melting, except during a short period at 1145°C where an irregularity briefly appeared. At 1115°C, the dissolution of Ni was completed in less than 3min and the total thickness dissolved was in the range 40–50μm. At 1145°C, the dissolution did not last much longer but the total thickness dissolved was significantly larger: approximately 180μm. At both temperatures, the velocity first increased, then reached a maximum value after 20–30s (0.6–0.8μm/s at 1115°C and 4.8μm/s at 1145°C), and finally tends progressively to zero. Post-mortem observations showed that the Ni was homogeneously dissolved over the entire sample height at 1115°C, which excludes any effects of convection on the velocities that we measured. On the contrary, at 1145°C, the dissolution was more important in the upper part of the sample and the interface appeared curved. The total thickness dissolved was in both cases larger than the predicted theoretical values and the melting velocities were also larger than the values obtained from finite difference calculations. The discrepancies are more pronounced at higher temperature.
•Solutal melting was investigated in-situ using laser scanning confocal microscopy.•The kinetics of the process in the Cu/Ni system was determined at 1115 and 1145°C.•A smooth and regular solid–liquid interface was observed.•The dissolution of Ni was completed in less than 3min at both temperatures.•The velocity increased, reached a maximum after 20–30s, and finally tends to zero.</description><identifier>ISSN: 1044-5803</identifier><identifier>EISSN: 1873-4189</identifier><identifier>DOI: 10.1016/j.matchar.2014.09.004</identifier><language>eng</language><publisher>New York, NY: Elsevier Inc</publisher><subject>Confocal ; Copper ; Cross-disciplinary physics: materials science; rheology ; DISSOLUTION ; Engineering Sciences ; Exact sciences and technology ; Laser scanning confocal microscopy ; LASERS ; Materials ; Materials science ; Melting ; MELTING POINT ; Microscopy ; Nickel ; Phase diagrams and microstructures developed by solidification and solid-solid phase transformations ; Physics ; Scanning ; Solidification ; Solutal melting</subject><ispartof>Materials characterization, 2014-11, Vol.97, p.125-131</ispartof><rights>2014 Elsevier Inc.</rights><rights>2015 INIST-CNRS</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c406t-9b46f600bc80b787d3ef681293274279e7a2d801cb81cbd0c5ef712e8a51c1a73</citedby><cites>FETCH-LOGICAL-c406t-9b46f600bc80b787d3ef681293274279e7a2d801cb81cbd0c5ef712e8a51c1a73</cites><orcidid>0000-0001-8061-7382 ; 0000-0001-9810-2360 ; 0000-0002-1722-2174 ; 0000-0002-5038-8029</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S1044580314002794$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,314,776,780,881,3537,27901,27902,65534</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=28888072$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-01291907$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Deillon, L.</creatorcontrib><creatorcontrib>Zollinger, J.</creatorcontrib><creatorcontrib>Daloz, D.</creatorcontrib><creatorcontrib>Založnik, M.</creatorcontrib><creatorcontrib>Combeau, H.</creatorcontrib><title>In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system</title><title>Materials characterization</title><description>Solutal melting was investigated in-situ by means of high temperature laser scanning confocal microscopy. This technique enabled us to track the motion of the solid–liquid interface in order to determine the evolution of the interfacial velocity. The Cu–Ni binary system was chosen as a model case and concentric samples were fabricated from both pure metals. Two holding temperatures above the melting point of Cu were investigated, i.e., 1115 and 1145°C. As the average composition of the mounted samples was chosen to lie within the solid solution region, the reaction occurred via the following steps: i) thermal melting of Cu, ii) solutal melting of Ni, and iii) resolidification. A smooth and regular s–l interface was observed during solutal melting, except during a short period at 1145°C where an irregularity briefly appeared. At 1115°C, the dissolution of Ni was completed in less than 3min and the total thickness dissolved was in the range 40–50μm. At 1145°C, the dissolution did not last much longer but the total thickness dissolved was significantly larger: approximately 180μm. At both temperatures, the velocity first increased, then reached a maximum value after 20–30s (0.6–0.8μm/s at 1115°C and 4.8μm/s at 1145°C), and finally tends progressively to zero. Post-mortem observations showed that the Ni was homogeneously dissolved over the entire sample height at 1115°C, which excludes any effects of convection on the velocities that we measured. On the contrary, at 1145°C, the dissolution was more important in the upper part of the sample and the interface appeared curved. The total thickness dissolved was in both cases larger than the predicted theoretical values and the melting velocities were also larger than the values obtained from finite difference calculations. The discrepancies are more pronounced at higher temperature.
•Solutal melting was investigated in-situ using laser scanning confocal microscopy.•The kinetics of the process in the Cu/Ni system was determined at 1115 and 1145°C.•A smooth and regular solid–liquid interface was observed.•The dissolution of Ni was completed in less than 3min at both temperatures.•The velocity increased, reached a maximum after 20–30s, and finally tends to zero.</description><subject>Confocal</subject><subject>Copper</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>DISSOLUTION</subject><subject>Engineering Sciences</subject><subject>Exact sciences and technology</subject><subject>Laser scanning confocal microscopy</subject><subject>LASERS</subject><subject>Materials</subject><subject>Materials science</subject><subject>Melting</subject><subject>MELTING POINT</subject><subject>Microscopy</subject><subject>Nickel</subject><subject>Phase diagrams and microstructures developed by solidification and solid-solid phase transformations</subject><subject>Physics</subject><subject>Scanning</subject><subject>Solidification</subject><subject>Solutal melting</subject><issn>1044-5803</issn><issn>1873-4189</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNqFkU2L2zAQhk1podttf0JBl0J7sHckO5bUS1lC210I7WV7FrI8bhRkKZXkQP79yiTstQJ98sw7o3mr6iOFhgLt7w7NrLPZ69gwoF0DsgHoXlU3VPC27qiQr8sZuq7eCGjfVu9SOgBALyi_qfaPvk42LyQMCeNJZxt8ImEiKbgla0dmdNn6v2RJ6-p0oUgy2vv1aoKfglkpa2JIJhzPX8nTHsl2uftlyRxGdCSdU8b5ffVm0i7hh-t-W_358f1p-1Dvfv983N7vatNBn2s5dP3UAwxGwMAFH1ucSqVMtox3jEvkmo0CqBlEmSOYDU6cMhR6Qw3VvL2tvlx099qpY7SzjmcVtFUP9zu1vkERoxL4iRb284U9xvBvwZTVbJNB57THsCRF-1JJKyVjBd1c0PWfKeL0ok1BrS6og7q6oFYXFEhVXChxn64pdOmam6L2xqaXYCbKAL7qf7twWHpzshhVMha9wdFGNFmNwf4n0zNFwqAX</recordid><startdate>20141101</startdate><enddate>20141101</enddate><creator>Deillon, L.</creator><creator>Zollinger, J.</creator><creator>Daloz, D.</creator><creator>Založnik, M.</creator><creator>Combeau, H.</creator><general>Elsevier Inc</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8G</scope><scope>JG9</scope><scope>L7M</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0001-8061-7382</orcidid><orcidid>https://orcid.org/0000-0001-9810-2360</orcidid><orcidid>https://orcid.org/0000-0002-1722-2174</orcidid><orcidid>https://orcid.org/0000-0002-5038-8029</orcidid></search><sort><creationdate>20141101</creationdate><title>In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system</title><author>Deillon, L. ; Zollinger, J. ; Daloz, D. ; Založnik, M. ; Combeau, H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c406t-9b46f600bc80b787d3ef681293274279e7a2d801cb81cbd0c5ef712e8a51c1a73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Confocal</topic><topic>Copper</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>DISSOLUTION</topic><topic>Engineering Sciences</topic><topic>Exact sciences and technology</topic><topic>Laser scanning confocal microscopy</topic><topic>LASERS</topic><topic>Materials</topic><topic>Materials science</topic><topic>Melting</topic><topic>MELTING POINT</topic><topic>Microscopy</topic><topic>Nickel</topic><topic>Phase diagrams and microstructures developed by solidification and solid-solid phase transformations</topic><topic>Physics</topic><topic>Scanning</topic><topic>Solidification</topic><topic>Solutal melting</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Deillon, L.</creatorcontrib><creatorcontrib>Zollinger, J.</creatorcontrib><creatorcontrib>Daloz, D.</creatorcontrib><creatorcontrib>Založnik, M.</creatorcontrib><creatorcontrib>Combeau, H.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Materials characterization</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Deillon, L.</au><au>Zollinger, J.</au><au>Daloz, D.</au><au>Založnik, M.</au><au>Combeau, H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system</atitle><jtitle>Materials characterization</jtitle><date>2014-11-01</date><risdate>2014</risdate><volume>97</volume><spage>125</spage><epage>131</epage><pages>125-131</pages><issn>1044-5803</issn><eissn>1873-4189</eissn><abstract>Solutal melting was investigated in-situ by means of high temperature laser scanning confocal microscopy. This technique enabled us to track the motion of the solid–liquid interface in order to determine the evolution of the interfacial velocity. The Cu–Ni binary system was chosen as a model case and concentric samples were fabricated from both pure metals. Two holding temperatures above the melting point of Cu were investigated, i.e., 1115 and 1145°C. As the average composition of the mounted samples was chosen to lie within the solid solution region, the reaction occurred via the following steps: i) thermal melting of Cu, ii) solutal melting of Ni, and iii) resolidification. A smooth and regular s–l interface was observed during solutal melting, except during a short period at 1145°C where an irregularity briefly appeared. At 1115°C, the dissolution of Ni was completed in less than 3min and the total thickness dissolved was in the range 40–50μm. At 1145°C, the dissolution did not last much longer but the total thickness dissolved was significantly larger: approximately 180μm. At both temperatures, the velocity first increased, then reached a maximum value after 20–30s (0.6–0.8μm/s at 1115°C and 4.8μm/s at 1145°C), and finally tends progressively to zero. Post-mortem observations showed that the Ni was homogeneously dissolved over the entire sample height at 1115°C, which excludes any effects of convection on the velocities that we measured. On the contrary, at 1145°C, the dissolution was more important in the upper part of the sample and the interface appeared curved. The total thickness dissolved was in both cases larger than the predicted theoretical values and the melting velocities were also larger than the values obtained from finite difference calculations. The discrepancies are more pronounced at higher temperature.
•Solutal melting was investigated in-situ using laser scanning confocal microscopy.•The kinetics of the process in the Cu/Ni system was determined at 1115 and 1145°C.•A smooth and regular solid–liquid interface was observed.•The dissolution of Ni was completed in less than 3min at both temperatures.•The velocity increased, reached a maximum after 20–30s, and finally tends to zero.</abstract><cop>New York, NY</cop><pub>Elsevier Inc</pub><doi>10.1016/j.matchar.2014.09.004</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0001-8061-7382</orcidid><orcidid>https://orcid.org/0000-0001-9810-2360</orcidid><orcidid>https://orcid.org/0000-0002-1722-2174</orcidid><orcidid>https://orcid.org/0000-0002-5038-8029</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1044-5803 |
ispartof | Materials characterization, 2014-11, Vol.97, p.125-131 |
issn | 1044-5803 1873-4189 |
language | eng |
recordid | cdi_hal_primary_oai_HAL_hal_01291907v1 |
source | Elsevier ScienceDirect Journals |
subjects | Confocal Copper Cross-disciplinary physics: materials science rheology DISSOLUTION Engineering Sciences Exact sciences and technology Laser scanning confocal microscopy LASERS Materials Materials science Melting MELTING POINT Microscopy Nickel Phase diagrams and microstructures developed by solidification and solid-solid phase transformations Physics Scanning Solidification Solutal melting |
title | In-situ observations of solutal melting using laser scanning confocal microscopy: The Cu/Ni model system |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-14T01%3A29%3A55IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_hal_p&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=In-situ%20observations%20of%20solutal%20melting%20using%20laser%20scanning%20confocal%20microscopy:%20The%20Cu/Ni%20model%20system&rft.jtitle=Materials%20characterization&rft.au=Deillon,%20L.&rft.date=2014-11-01&rft.volume=97&rft.spage=125&rft.epage=131&rft.pages=125-131&rft.issn=1044-5803&rft.eissn=1873-4189&rft_id=info:doi/10.1016/j.matchar.2014.09.004&rft_dat=%3Cproquest_hal_p%3E1660039922%3C/proquest_hal_p%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1660039922&rft_id=info:pmid/&rft_els_id=S1044580314002794&rfr_iscdi=true |