Jianhao Wang, Cai Chen, Yuanxun Zhou, Zheyu Wu, Xingyu Gao, Bingbing Zhao, Lanting Zhang, Hong Wang
{"title":"An in-situ high-throughput study of the Invar effect in the Fe–Ni–Co system","authors":"Jianhao Wang, Cai Chen, Yuanxun Zhou, Zheyu Wu, Xingyu Gao, Bingbing Zhao, Lanting Zhang, Hong Wang","doi":"10.1016/j.jallcom.2024.177755","DOIUrl":null,"url":null,"abstract":"The Fe–Ni based classical Invar alloy and the Fe–Ni–Co based super Invar alloy are the basis for designing multicomponent alloys with low thermal expansion. In this work, we applied in-situ high-throughput experimental methods to map chemical composition, crystal structure, coefficient of thermal expansion (CTE) and magnetism in the Fe–Ni–Co system. The distribution of CTE (80~200℃) measured by the in-situ micro-beam X-ray diffraction on the combinatorial materials chips (CMC) showed low CTE regions in agreement with previous reports. Combined with the MOKE measurements, the <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">&#x3BC;</mi></mrow><mo is=\"true\">&#x305;</mo></mover><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">&#x2212;</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">&#x305;</mo></mover></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -647.8 2336.1 947.9\" width=\"5.426ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(108,-35)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\" transform=\"translate(825,0)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(1826,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g></g><g is=\"true\" transform=\"translate(68,-34)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mo is=\"true\" linebreak=\"badbreak\" linebreakstyle=\"after\">−</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">−</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></script></span> relation of the Fe–Ni–Co ternary FCC phase is found to follow the reported FCC Fe–Ni alloys in the Slater-Pauling curve. A low CTE region is centred at <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">&#x305;</mo></mover></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.74ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.208ex;\" viewbox=\"0 -647.8 509.6 749.2\" width=\"1.184ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g></g><g is=\"true\" transform=\"translate(68,-34)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></script></span> = 26.7 and <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">&#x3BC;</mi></mrow><mo is=\"true\">&#x305;</mo></mover><mspace width=\"1em\" is=\"true\" /></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -647.8 1603.5 947.9\" width=\"3.724ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(108,-35)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\"></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mspace is=\"true\" width=\"1em\"></mspace></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mspace width=\"1em\" is=\"true\"></mspace></math></script></span>= 1.26 <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">&#x3BC;</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.971ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -498.8 1240.5 848.5\" width=\"2.881ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(603,-253)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-42\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">μ</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">μ</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math></script></span> in the Slater-Pauling curve. The observed low CTE zone not only matches with the classical Invar and super Invar alloys but also agrees with the reported Fe–Ni–Co based multicomponent alloys with a small amount of doping (< 5<!-- --> <!-- -->at.%) by Cu, Cr, Mn etc. The effect of Cr addition (> 5<!-- --> <!-- -->at.%) to Fe–Ni–Co alloys on the Invar effect is further discussed in terms of the interplay between magnetism and austinite stability.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"15 1","pages":""},"PeriodicalIF":5.8000,"publicationDate":"2024-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2024.177755","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The Fe–Ni based classical Invar alloy and the Fe–Ni–Co based super Invar alloy are the basis for designing multicomponent alloys with low thermal expansion. In this work, we applied in-situ high-throughput experimental methods to map chemical composition, crystal structure, coefficient of thermal expansion (CTE) and magnetism in the Fe–Ni–Co system. The distribution of CTE (80~200℃) measured by the in-situ micro-beam X-ray diffraction on the combinatorial materials chips (CMC) showed low CTE regions in agreement with previous reports. Combined with the MOKE measurements, the relation of the Fe–Ni–Co ternary FCC phase is found to follow the reported FCC Fe–Ni alloys in the Slater-Pauling curve. A low CTE region is centred at = 26.7 and = 1.26 in the Slater-Pauling curve. The observed low CTE zone not only matches with the classical Invar and super Invar alloys but also agrees with the reported Fe–Ni–Co based multicomponent alloys with a small amount of doping (< 5 at.%) by Cu, Cr, Mn etc. The effect of Cr addition (> 5 at.%) to Fe–Ni–Co alloys on the Invar effect is further discussed in terms of the interplay between magnetism and austinite stability.
期刊介绍:
The Journal of Alloys and Compounds is intended to serve as an international medium for the publication of work on solid materials comprising compounds as well as alloys. Its great strength lies in the diversity of discipline which it encompasses, drawing together results from materials science, solid-state chemistry and physics.