Nd-Fe-B合金的高温氢致相变

IF 6.3 2区 材料科学 Q2 CHEMISTRY, PHYSICAL
G. BACCHETTA, F. ORLANDINI-KELLER, C. FLAMENT, L. MAGNIER, S. LUCA, C. RADO, J.P. GARANDET
{"title":"Nd-Fe-B合金的高温氢致相变","authors":"G. BACCHETTA, F. ORLANDINI-KELLER, C. FLAMENT, L. MAGNIER, S. LUCA, C. RADO, J.P. GARANDET","doi":"10.1016/j.jallcom.2024.177980","DOIUrl":null,"url":null,"abstract":"The disproportionation of Nd-Fe-B alloys has been thoroughly studied in connection with its importance in the well-known Hydrogenation Disproportionation Desorption Recombination (HDDR) process. However, little attention has been paid to the Dy containing Nd-Fe-B alloys. We present here a study of the evolution of the microstructure according to the disproportionation temperature on both Dy-rich and Dy-free Nd-Fe-B based alloys. Thanks to a combined implementation of XRD, SEM, TEM and WDS-EDS techniques, we could evidence that, under a hydrogen pressure of 80 kPa, a partial recombination occurs at high temperature prior to the full desorption of hydrogen and the complete recombination of the alloy. A phase transformation of the type <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;REH&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;mo is=\"true\"&gt;&amp;#xB1;&lt;/mo&gt;&lt;mi is=\"true\"&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\"&gt;+&lt;/mo&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;Fe&lt;/mi&gt;&lt;mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\"&gt;+&lt;/mo&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;Fe&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi is=\"true\"&gt;B&lt;/mi&gt;&lt;mo is=\"true\"&gt;&amp;#x2192;&lt;/mo&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;RE&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;1&lt;/mn&gt;&lt;mo is=\"true\"&gt;+&lt;/mo&gt;&lt;mi is=\"true\"&gt;&amp;#x3B5;&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;Fe&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi is=\"true\"&gt;B&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\"&gt;+&lt;/mo&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;RE&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi mathvariant=\"italic\" is=\"true\"&gt;Fe&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;14&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi is=\"true\"&gt;B&lt;/mi&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.432ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -747.2 22635.8 1047.3\" width=\"52.574ex\" 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-52\"></use><use x=\"759\" xlink:href=\"#MJMATHI-45\" y=\"0\"></use><use x=\"1498\" xlink:href=\"#MJMATHI-48\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(2329,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-32\"></use></g><g is=\"true\" transform=\"translate(353,0)\"><use 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is=\"true\" transform=\"translate(21876,0)\"><use xlink:href=\"#MJMATHI-42\"></use></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\">REH</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn><mo is=\"true\">±</mo><mi is=\"true\">x</mi></mrow></msub><mo is=\"true\" linebreak=\"badbreak\" linebreakstyle=\"after\">+</mo><mi is=\"true\" mathvariant=\"italic\">Fe</mi><mo is=\"true\" linebreak=\"badbreak\" linebreakstyle=\"after\">+</mo><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msub><mi is=\"true\">B</mi><mo is=\"true\">→</mo><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">RE</mi></mrow><mrow is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">+</mo><mi is=\"true\">ε</mi></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">B</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub><mo is=\"true\" linebreak=\"badbreak\" linebreakstyle=\"after\">+</mo><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">RE</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">14</mn></mrow></msub><mi is=\"true\">B</mi></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">REH</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn><mo is=\"true\">±</mo><mi is=\"true\">x</mi></mrow></msub><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">+</mo><mi mathvariant=\"italic\" is=\"true\">Fe</mi><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">+</mo><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msub><mi is=\"true\">B</mi><mo is=\"true\">→</mo><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">RE</mi></mrow><mrow is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">+</mo><mi is=\"true\">ε</mi></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\">B</mi></mrow><mrow is=\"true\"><mn is=\"true\">4</mn></mrow></msub><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">+</mo><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">RE</mi></mrow><mrow is=\"true\"><mn is=\"true\">2</mn></mrow></msub><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">Fe</mi></mrow><mrow is=\"true\"><mn is=\"true\">14</mn></mrow></msub><mi is=\"true\">B</mi></math></script></span> is evidenced at high temperature, where RE (Rare Earth) stands for either Nd, Pr or Dy. To the best of our knowledge such a phase transformation has not been previously reported in the literature. This phase equilibrium occurs simultaneously with a coarsening of the microstructure. The phase transformation temperatures are identified by a TGA/DTA analysis. It points to a dependence of the extension of the stability domain of this newly referenced phase equilibrium on the Dy-content in the initial alloy. This study paves the way for the determination of phase diagrams under hydrogen for Nd-Fe-B alloys.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"19 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2024-12-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"High-temperature hydrogen-induced phase transformation in Nd-Fe-B alloys\",\"authors\":\"G. BACCHETTA, F. ORLANDINI-KELLER, C. FLAMENT, L. MAGNIER, S. LUCA, C. RADO, J.P. GARANDET\",\"doi\":\"10.1016/j.jallcom.2024.177980\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The disproportionation of Nd-Fe-B alloys has been thoroughly studied in connection with its importance in the well-known Hydrogenation Disproportionation Desorption Recombination (HDDR) process. However, little attention has been paid to the Dy containing Nd-Fe-B alloys. We present here a study of the evolution of the microstructure according to the disproportionation temperature on both Dy-rich and Dy-free Nd-Fe-B based alloys. Thanks to a combined implementation of XRD, SEM, TEM and WDS-EDS techniques, we could evidence that, under a hydrogen pressure of 80 kPa, a partial recombination occurs at high temperature prior to the full desorption of hydrogen and the complete recombination of the alloy. A phase transformation of the type <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi mathvariant=\\\"italic\\\" is=\\\"true\\\"&gt;REH&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB1;&lt;/mo&gt;&lt;mi is=\\\"true\\\"&gt;x&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\" is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;mi mathvariant=\\\"italic\\\" is=\\\"true\\\"&gt;Fe&lt;/mi&gt;&lt;mo linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\" is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi mathvariant=\\\"italic\\\" is=\\\"true\\\"&gt;Fe&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi is=\\\"true\\\"&gt;B&lt;/mi&gt;&lt;mo 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is=\\\"true\\\"&gt;RE&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi mathvariant=\\\"italic\\\" is=\\\"true\\\"&gt;Fe&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;14&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mi is=\\\"true\\\"&gt;B&lt;/mi&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.432ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -747.2 22635.8 1047.3\\\" width=\\\"52.574ex\\\" 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 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mathvariant=\\\"italic\\\">Fe</mi></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">4</mn></mrow></msub><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">B</mi></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">4</mn></mrow></msub><mo is=\\\"true\\\" linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\">+</mo><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\" mathvariant=\\\"italic\\\">RE</mi></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow></msub><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\" mathvariant=\\\"italic\\\">Fe</mi></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">14</mn></mrow></msub><mi is=\\\"true\\\">B</mi></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi mathvariant=\\\"italic\\\" is=\\\"true\\\">REH</mi></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn><mo is=\\\"true\\\">±</mo><mi is=\\\"true\\\">x</mi></mrow></msub><mo linebreak=\\\"badbreak\\\" 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引用次数: 0

摘要

由于钕铁硼合金的歧化在众所周知的氢化歧化解吸重组(HDDR)过程中具有重要意义,因此对其进行了深入研究。然而,人们很少关注含镝的钕铁硼合金。我们在此介绍根据富钕铁硼合金和无钕铁硼合金的歧化温度对微观结构演变的研究。通过结合使用 XRD、SEM、TEM 和 WDS-EDS 技术,我们可以证明,在 80 kPa 的氢气压力下,合金在完全解吸氢气和完全重组之前,会在高温下发生部分重组。在高温下发生了 REH2±x+Fe+Fe2B→RE1+εFe4B4+RE2Fe14BREH2±x+Fe+Fe2B→RE1+εFe4B4+RE2Fe14B 类型的相变,其中 RE(稀土)代表 Nd、Pr 或 Dy。据我们所知,这种相变以前从未在文献中报道过。这种相平衡与微观结构的粗化同时发生。相变温度是通过 TGA/DTA 分析确定的。它指出这种新引用的相平衡的稳定域的扩展取决于初始合金中的镝含量。这项研究为确定 Nd-Fe-B 合金在氢气条件下的相图铺平了道路。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
High-temperature hydrogen-induced phase transformation in Nd-Fe-B alloys
The disproportionation of Nd-Fe-B alloys has been thoroughly studied in connection with its importance in the well-known Hydrogenation Disproportionation Desorption Recombination (HDDR) process. However, little attention has been paid to the Dy containing Nd-Fe-B alloys. We present here a study of the evolution of the microstructure according to the disproportionation temperature on both Dy-rich and Dy-free Nd-Fe-B based alloys. Thanks to a combined implementation of XRD, SEM, TEM and WDS-EDS techniques, we could evidence that, under a hydrogen pressure of 80 kPa, a partial recombination occurs at high temperature prior to the full desorption of hydrogen and the complete recombination of the alloy. A phase transformation of the type REH2±x+Fe+Fe2BRE1+εFe4B4+RE2Fe14B is evidenced at high temperature, where RE (Rare Earth) stands for either Nd, Pr or Dy. To the best of our knowledge such a phase transformation has not been previously reported in the literature. This phase equilibrium occurs simultaneously with a coarsening of the microstructure. The phase transformation temperatures are identified by a TGA/DTA analysis. It points to a dependence of the extension of the stability domain of this newly referenced phase equilibrium on the Dy-content in the initial alloy. This study paves the way for the determination of phase diagrams under hydrogen for Nd-Fe-B alloys.
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来源期刊
Journal of Alloys and Compounds
Journal of Alloys and Compounds 工程技术-材料科学:综合
CiteScore
11.10
自引率
14.50%
发文量
5146
审稿时长
67 days
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.
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