Carbon Diffusion in Lanthanum Erbium Carbide Stabilized in the Cubic Fluorite Structure
Lanthanum erbium carbide, La 0.5 Er 0.5 C 2 , a salt-like carbide with a cubic fluorite phase structure, has been produced from 13 C, allowing carbon diffusion rate to be determined using 12 C. Carbon in salt-like carbides exhibits significant ionicity, and a high carbon diffusion rate would enable...
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creator | Simmons, W. Neal Cocks, Franklin Hadley |
description | Lanthanum erbium carbide, La
0.5
Er
0.5
C
2
, a salt-like carbide with a cubic fluorite phase structure, has been produced from
13
C, allowing carbon diffusion rate to be determined using
12
C. Carbon in salt-like carbides exhibits significant ionicity, and a high carbon diffusion rate would enable a new class of high temperature fuel cells based on carbon-ion transport. The complete lack of carbon diffusion data for salt-like carbides is the motivation for this work. The carbon diffusion rate in La
0.5
Er
0.5
C
2
has now been determined to be 2.0 ± 0.8 × 10
−13
cm
2
/s at 850 °C, increasing to 1.8 ± 0.8 × 10
−11
cm
2
/s at 1150 °C, with an activation energy of about 95 kJ/mole. These diffusion rates are too low for a carbon-ion fuel cell, but a number of other salt-like carbides exist. Be
2
C, in particular, is a salt-like carbide with an antifluorite structure, and should have higher carbon-ion diffusion than cubic La
0.5
Er
0.5
C
2
due to the unoccupied octahedral sites in the antifluorite structure, but Be
2
C presents special difficulties due to the toxic nature of its hydrolysis products. |
doi_str_mv | 10.1007/s11669-012-0003-6 |
format | Article |
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0.5
Er
0.5
C
2
, a salt-like carbide with a cubic fluorite phase structure, has been produced from
13
C, allowing carbon diffusion rate to be determined using
12
C. Carbon in salt-like carbides exhibits significant ionicity, and a high carbon diffusion rate would enable a new class of high temperature fuel cells based on carbon-ion transport. The complete lack of carbon diffusion data for salt-like carbides is the motivation for this work. The carbon diffusion rate in La
0.5
Er
0.5
C
2
has now been determined to be 2.0 ± 0.8 × 10
−13
cm
2
/s at 850 °C, increasing to 1.8 ± 0.8 × 10
−11
cm
2
/s at 1150 °C, with an activation energy of about 95 kJ/mole. These diffusion rates are too low for a carbon-ion fuel cell, but a number of other salt-like carbides exist. Be
2
C, in particular, is a salt-like carbide with an antifluorite structure, and should have higher carbon-ion diffusion than cubic La
0.5
Er
0.5
C
2
due to the unoccupied octahedral sites in the antifluorite structure, but Be
2
C presents special difficulties due to the toxic nature of its hydrolysis products.</description><identifier>ISSN: 1547-7037</identifier><identifier>EISSN: 1863-7345</identifier><identifier>EISSN: 1934-7243</identifier><identifier>DOI: 10.1007/s11669-012-0003-6</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Ceramics ; Composites ; Crystallography and Scattering Methods ; Engineering Thermodynamics ; Glass ; Heat and Mass Transfer ; Metallic Materials ; Natural Materials ; Physics ; Physics and Astronomy ; Short Communication ; Thermodynamics</subject><ispartof>Journal of phase equilibria and diffusion, 2012-04, Vol.33 (2), p.85-88</ispartof><rights>ASM International 2012</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c315t-a745cd0d2df40351c4e0f2c60ec3872b4b8ea33de527656155fee5326dab8ebc3</citedby><cites>FETCH-LOGICAL-c315t-a745cd0d2df40351c4e0f2c60ec3872b4b8ea33de527656155fee5326dab8ebc3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11669-012-0003-6$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11669-012-0003-6$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,41467,42536,51297</link.rule.ids></links><search><creatorcontrib>Simmons, W. Neal</creatorcontrib><creatorcontrib>Cocks, Franklin Hadley</creatorcontrib><title>Carbon Diffusion in Lanthanum Erbium Carbide Stabilized in the Cubic Fluorite Structure</title><title>Journal of phase equilibria and diffusion</title><addtitle>J. Phase Equilib. Diffus</addtitle><description>Lanthanum erbium carbide, La
0.5
Er
0.5
C
2
, a salt-like carbide with a cubic fluorite phase structure, has been produced from
13
C, allowing carbon diffusion rate to be determined using
12
C. Carbon in salt-like carbides exhibits significant ionicity, and a high carbon diffusion rate would enable a new class of high temperature fuel cells based on carbon-ion transport. The complete lack of carbon diffusion data for salt-like carbides is the motivation for this work. The carbon diffusion rate in La
0.5
Er
0.5
C
2
has now been determined to be 2.0 ± 0.8 × 10
−13
cm
2
/s at 850 °C, increasing to 1.8 ± 0.8 × 10
−11
cm
2
/s at 1150 °C, with an activation energy of about 95 kJ/mole. These diffusion rates are too low for a carbon-ion fuel cell, but a number of other salt-like carbides exist. Be
2
C, in particular, is a salt-like carbide with an antifluorite structure, and should have higher carbon-ion diffusion than cubic La
0.5
Er
0.5
C
2
due to the unoccupied octahedral sites in the antifluorite structure, but Be
2
C presents special difficulties due to the toxic nature of its hydrolysis products.</description><subject>Ceramics</subject><subject>Composites</subject><subject>Crystallography and Scattering Methods</subject><subject>Engineering Thermodynamics</subject><subject>Glass</subject><subject>Heat and Mass Transfer</subject><subject>Metallic Materials</subject><subject>Natural Materials</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Short Communication</subject><subject>Thermodynamics</subject><issn>1547-7037</issn><issn>1863-7345</issn><issn>1934-7243</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNp1kEtLxDAUhYMoOI7-AHfFffQmaZJ2KXV8wIALFZchTVMnw0w75rHQX29KBVeuzoH7nXPhIHRJ4JoAyJtAiBA1BkIxADAsjtCCVIJhyUp-nD0vJZbA5Ck6C2ELQGtZiQV6b7Rvx6G4c32fgsvODcVaD3Gjh7QvVr51WSbIdbZ4ibp1O_dtuwmLG1s0qXWmuN-l0bs4AT6ZmLw9Rye93gV78atL9Ha_em0e8fr54am5XWPDCI9Yy5KbDjra9SUwTkxpoadGgDWskrQt28pqxjrLqRRcEM57azmjotP50hq2RFdz78GPn8mGqLZj8kN-qWpJSF2CpBkiM2T8GIK3vTp4t9f-SxFQ03xqnk_l-dQ0nxI5Q-dMyOzwYf1f8f-hH-m3crE</recordid><startdate>20120401</startdate><enddate>20120401</enddate><creator>Simmons, W. Neal</creator><creator>Cocks, Franklin Hadley</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7RQ</scope><scope>7U5</scope><scope>7XB</scope><scope>8BQ</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>KB.</scope><scope>L7M</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>Q9U</scope><scope>U9A</scope></search><sort><creationdate>20120401</creationdate><title>Carbon Diffusion in Lanthanum Erbium Carbide Stabilized in the Cubic Fluorite Structure</title><author>Simmons, W. Neal ; Cocks, Franklin Hadley</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c315t-a745cd0d2df40351c4e0f2c60ec3872b4b8ea33de527656155fee5326dab8ebc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Ceramics</topic><topic>Composites</topic><topic>Crystallography and Scattering Methods</topic><topic>Engineering Thermodynamics</topic><topic>Glass</topic><topic>Heat and Mass Transfer</topic><topic>Metallic Materials</topic><topic>Natural Materials</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Short Communication</topic><topic>Thermodynamics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Simmons, W. Neal</creatorcontrib><creatorcontrib>Cocks, Franklin Hadley</creatorcontrib><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Career & Technical Education Database</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>Materials Science Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Materials Science Collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>ProQuest Central Basic</collection><jtitle>Journal of phase equilibria and diffusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Simmons, W. Neal</au><au>Cocks, Franklin Hadley</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Carbon Diffusion in Lanthanum Erbium Carbide Stabilized in the Cubic Fluorite Structure</atitle><jtitle>Journal of phase equilibria and diffusion</jtitle><stitle>J. Phase Equilib. Diffus</stitle><date>2012-04-01</date><risdate>2012</risdate><volume>33</volume><issue>2</issue><spage>85</spage><epage>88</epage><pages>85-88</pages><issn>1547-7037</issn><eissn>1863-7345</eissn><eissn>1934-7243</eissn><abstract>Lanthanum erbium carbide, La
0.5
Er
0.5
C
2
, a salt-like carbide with a cubic fluorite phase structure, has been produced from
13
C, allowing carbon diffusion rate to be determined using
12
C. Carbon in salt-like carbides exhibits significant ionicity, and a high carbon diffusion rate would enable a new class of high temperature fuel cells based on carbon-ion transport. The complete lack of carbon diffusion data for salt-like carbides is the motivation for this work. The carbon diffusion rate in La
0.5
Er
0.5
C
2
has now been determined to be 2.0 ± 0.8 × 10
−13
cm
2
/s at 850 °C, increasing to 1.8 ± 0.8 × 10
−11
cm
2
/s at 1150 °C, with an activation energy of about 95 kJ/mole. These diffusion rates are too low for a carbon-ion fuel cell, but a number of other salt-like carbides exist. Be
2
C, in particular, is a salt-like carbide with an antifluorite structure, and should have higher carbon-ion diffusion than cubic La
0.5
Er
0.5
C
2
due to the unoccupied octahedral sites in the antifluorite structure, but Be
2
C presents special difficulties due to the toxic nature of its hydrolysis products.</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1007/s11669-012-0003-6</doi><tpages>4</tpages></addata></record> |
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subjects | Ceramics Composites Crystallography and Scattering Methods Engineering Thermodynamics Glass Heat and Mass Transfer Metallic Materials Natural Materials Physics Physics and Astronomy Short Communication Thermodynamics |
title | Carbon Diffusion in Lanthanum Erbium Carbide Stabilized in the Cubic Fluorite Structure |
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