Article(id=1321511462913290937, tenantId=1146029695717560320, journalId=1220038251117760515, issueId=1321508707721138247, articleNumber=null, orderNo=null, doi=10.11868/j.issn.1001-4381.2023.000668, pmid=null, cstr=32421.14.j.issn.1001-4381.2023.000668, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=research-article, receivedDate=1696694400000, receivedDateStr=2023-10-08, revisedDate=null, revisedDateStr=null, acceptedDate=1726675200000, acceptedDateStr=2024-09-19, onlineDate=1793002485253, onlineDateStr=2026-10-26, pubDate=1766160000000, pubDateStr=2025-12-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1793002485253, onlineIssueDateStr=2026-10-26, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1793002485253, creator=13701087609, updateTime=1793002485253, updator=13701087609, issue=Issue{id=1321508707721138247, tenantId=1146029695717560320, journalId=1220038251117760515, year='2025', volume='53', issue='12', pageStart='1', pageEnd='296', issueExtLink='null', onlineDate='null', pubDate='1766160000000', pubDateStr='2025-12-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1793001828365, creator='13701087609', updateTime=1793001828365, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext=null, issueFiles=null, downloadFileDto=null}, startPage=200, endPage=207, ext={EN=ArticleExt(id=1321511463102034618, articleId=1321511462913290937, tenantId=1146029695717560320, journalId=1220038251117760515, language=EN, title=Thermodynamic calculation of phase diagrams for Al-C-X(X=Mo,Nb,Ta,V), columnId=1220689384450478826, journalTitle=Journal of Materials Engineering, columnName=RESEARCH ARTICLE, runingTitle=null, highlight=null, articleAbstract=

The Al-C-X(X=Mo,Nb,Ta,V) systems are studied by CALPHAD (calculation of phase diagrams) coupled with first-principles calculations. Two ternary phases,Ta5Al3C and Ta2AlC are identified in the Al-C-Ta system. All of the other three systems exist only one stable ternary phase, Mo3Al2C for Al-C-Mo, Nb2AlC for Al-C-Nb, and V2AlC for Al-C-V, respectively. The enthalpies of formation of these compounds are obtained by First-principles calculations, and their Gibbs free energies are presented by stoichiometric models. Finally, a series of self-consistent thermodynamic parameters are derived by CALPHAD method. The optimized isothermal sections and thermodynamic properties are in good agreement with experimental and computational results. The Al-C-X (X=Mo,Nb,Ta,V) systems assessed in this work can help to establish a thermodynamic database of hard alloys with precipitation strengthening bonding phases, which will be used to guide the design of new materials with excellent properties.

, authors=Chuang SHI, Xin XIA, Weibin ZHANG, Weili WANG, Guifang HAN, Hongyu GONG, Jingde ZHANG, authorsList=Chuang SHI, Xin XIA, Weibin ZHANG, Weili WANG, Guifang HAN, Hongyu GONG, Jingde ZHANG, authorCompany=null, correspAuthors=Weibin ZHANG, authorNote=null, correspAuthorsNote=null, copyrightStatement=null, copyrightOwner=null, extLink=null, articleAbsUrl=null, sourceXml=null, magXml=null, pdfUrl=null, pdf=null, pdfFileSize=null, pdfExtLink=null, richHtmlUrl=null, mobilePdfUrl=null, reviewReport=null, pdfFirstPage=null, abstractGraph=null, abstractGraphContent=null, abstractVideo=null, citation=null, cebUrl=null, magXmlContent=null, mapNumber=null, fund=null), CN=ArticleExt(id=1321511464561652425, articleId=1321511462913290937, tenantId=1146029695717560320, journalId=1220038251117760515, language=CN, title=Al-C-X(X=Mo,Nb,Ta,V)的相图热力学计算, columnId=1220689384622445292, journalTitle=材料工程, columnName=研究论文, runingTitle=null, highlight=null, articleAbstract=

采用相图计算(calculation of phase diagrams, CALPHAD)耦合第一性原理计算对Al-C-X(X=Mo,Nb,Ta,V)体系进行了热力学研究。Al-C-Mo、Al-C-Nb和Al-C-V体系都只存在一个三元热力学稳定相,分别是Mo3Al2C、Nb2AlC和V2AlC。Al-C-Ta体系中的三元化合物为Ta5Al3C和Ta2AlC。通过第一性原理计算得到了这些化合物的生成焓,采用线性化合物模型描述其吉布斯自由能,最终由CALPHAD方法得到了一系列自洽的热力学参数。研究表明:优化得到的等温截面图和热力学数据与实验和计算结果均十分吻合。Al-C-X(X=Mo,Nb,Ta,V)体系的热力学参数能够帮助建立起析出强化黏结相的硬质合金数据库,指导设计具有优异性能的新型材料。

, authors=石闯, 夏新, 张伟彬, 王伟礼, 韩桂芳, 龚红宇, 张景德, authorsList=石闯, 夏新, 张伟彬, 王伟礼, 韩桂芳, 龚红宇, 张景德, authorCompany=null, correspAuthors=张伟彬, authorNote=null, correspAuthorsNote=
张伟彬(1985—),男,教授,博士,研究方向为硬质合金材料设计与产品研发,联系地址:山东省济南市历下区山东大学千佛山校区材料科学与工程学院(250061),E-mail:
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Journal of Alloys and Compounds, 2016, 666:279-286., articleTitle=Stability of V2AlC with Al in 800-1000 ℃ temperature range and in situ synthesis of V2AlC/Al composites, refAbstract=null)], funds=[Fund(id=1321926677261832288, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, awardId=2023YFB3712600, language=CN, fundingSource=国家重点研发计划(2023YFB3712600), fundOrder=null, country=null), Fund(id=1321926677337329761, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, awardId=52171009, language=CN, fundingSource=国家自然科学基金(52171009), fundOrder=null, country=null)], companyList=[AuthorCompany(id=1321926662665654299, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, xref=null, ext=[AuthorCompanyExt(id=1321926662686625820, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, companyId=1321926662665654299, language=EN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=Key Laboratory for Liquid-Solid Structural Evolution and Processing of Materials (Ministry of Education),Shandong University,Jinan 250061,China), AuthorCompanyExt(id=1321926662703403037, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, companyId=1321926662665654299, language=CN, country=null, province=null, city=null, postcode=null, companyName=null, departmentName=null, remark=山东大学 材料液固结构演化与加工重点 实验室(教育部),济南 250061)])], figs=[ArticleFig(id=1321926673558261837, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.1, caption=Calculated standard enthalpies of formation for the Al-C-X(X=Mo,Nb,Ta,V) ternary compounds along with the literature data[31], figureFileSmall=1tl67C64jF4n4ZOW5dU+OQ==, figureFileBig=j4I4snzV5CgREEvC/9mDVw==, tableContent=null), ArticleFig(id=1321926673856057422, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图1, caption=计算的Al-C-X (X=Mo, Nb, Ta, V)体系中三元化合物的标准生成焓和文献对比[31], figureFileSmall=1tl67C64jF4n4ZOW5dU+OQ==, figureFileBig=j4I4snzV5CgREEvC/9mDVw==, tableContent=null), ArticleFig(id=1321926673956720719, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.2, caption=Calculated isothermal section of Al-C-Mo system at 1450 ℃(a) and 1000 ℃(b), figureFileSmall=mukCeQFTIQgf1oPMBmuOug==, figureFileBig=o6Yu0zPWVxSYruTMEPsK+w==, tableContent=null), ArticleFig(id=1321926674246127696, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图2, caption=Al-C-Mo体系在1450 ℃(a)及1000 ℃(b)的等温截面图, figureFileSmall=mukCeQFTIQgf1oPMBmuOug==, figureFileBig=o6Yu0zPWVxSYruTMEPsK+w==, tableContent=null), ArticleFig(id=1321926675911266386, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.3, caption=Calculated isothermal section of the Al-C-Nb system at 700 ℃(a) and 1000 ℃(b), figureFileSmall=mM5uCDsAmSZkRl+RwAnjcg==, figureFileBig=APUacsBPpL2oOCq2yXzMnQ==, tableContent=null), ArticleFig(id=1321926676020318291, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图3, caption=Al-C-Nb体系在700 ℃ (a)及1000 ℃ (b)的等温截面图, figureFileSmall=mM5uCDsAmSZkRl+RwAnjcg==, figureFileBig=APUacsBPpL2oOCq2yXzMnQ==, tableContent=null), ArticleFig(id=1321926676095815764, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.4, caption=Calculated heat capacity of Ta2AlC compound along with the literature data[30], figureFileSmall=BCH3TfBesXy1skg89NSruA==, figureFileBig=0LLWtxPEe/8qZQmtpN6u5A==, tableContent=null), ArticleFig(id=1321926676175507541, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图4, caption=计算的化合物Ta2AlC的热容和文献数据[30], figureFileSmall=BCH3TfBesXy1skg89NSruA==, figureFileBig=0LLWtxPEe/8qZQmtpN6u5A==, tableContent=null), ArticleFig(id=1321926676234227798, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.5, caption=Calculated isothermal section of the Al-C-Ta system at 700 ℃(a) and 1000 ℃(b), figureFileSmall=26PT53IS5SJtYQf2QbaYYw==, figureFileBig=8njzPkOXhgDALK3fHQdVvg==, tableContent=null), ArticleFig(id=1321926676318113879, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图5, caption=Al-C-Ta体系在700 ℃(a)和1000 ℃(b)的等温截面图, figureFileSmall=26PT53IS5SJtYQf2QbaYYw==, figureFileBig=8njzPkOXhgDALK3fHQdVvg==, tableContent=null), ArticleFig(id=1321926676410388568, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.6, caption=Calculated heat capacity of V2AlC compound along with the literature data[31], figureFileSmall=JYsIDDHvK5RTKFNfDnWMkA==, figureFileBig=2790jLROYBNuRiQcZQZAKA==, tableContent=null), ArticleFig(id=1321926676469108825, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图6, caption=计算的化合物V2AlC的热容和文献数据[31], figureFileSmall=JYsIDDHvK5RTKFNfDnWMkA==, figureFileBig=2790jLROYBNuRiQcZQZAKA==, tableContent=null), ArticleFig(id=1321926676544606298, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Fig.7, caption=Calculated isothermal section of the Al-C-V system at 800 ℃(a) and 1000 ℃(b)[45], figureFileSmall=W61Q9dGB3c/4SUEtNjsEng==, figureFileBig=CVOI5gWvNa2Vpq//uDK0zA==, tableContent=null), ArticleFig(id=1321926676636880987, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=图7, caption=Al-C-V体系在800 ℃(a)和1000 ℃(b)的等温截面图[45], figureFileSmall=W61Q9dGB3c/4SUEtNjsEng==, figureFileBig=CVOI5gWvNa2Vpq//uDK0zA==, tableContent=null), ArticleFig(id=1321926676750127196, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Table 1, caption=

Crystal information and formation enthalpy of ternary phases in the Al-C-X(X=Mo,Nb,Ta,V) systems[27-29,31]

, figureFileSmall=null, figureFileBig=null, tableContent=
SystemPhasePearson symbolSpace groupPrototypeLattice parameter

ΔHf/

(kJ∙mol-1∙atom-1)

Ref.
a/nmb/nmc/nm
Al-C-MoMo3Al2CcP24P4132β-Mn0.68600.68600.6860[27]
0.68760.68760.6876-24.132This work
Al-C-NbNb2AlChP8P63/mmcCr2AlC0.31050.31051.3890[28]
0.31090.31091.3920-61.168This work
Al-C-TaTa2AlChP8P63/mmcCr2AlC0.30750.30751.3830[28]
0.30900.30901.3962-56.071This work
Ta5Al3ChP16P63/mcmβ-Mn5Si30.52450.52450.7734[28]
0.53310.53310.7792-38.484This work
Al-C-VV2AlChP8P63/mmcCr2AlC0.29110.29111.3140[29]
-47.08±3.53[31]
0.28920.28921.3176-51.750This work
), ArticleFig(id=1321926676825624669, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=表1, caption=

Al-C-X(X=Mo,Nb,Ta,V)体系中三元化合物的晶体信息和生成焓[27-29,31]

, figureFileSmall=null, figureFileBig=null, tableContent=
SystemPhasePearson symbolSpace groupPrototypeLattice parameter

ΔHf/

(kJ∙mol-1∙atom-1)

Ref.
a/nmb/nmc/nm
Al-C-MoMo3Al2CcP24P4132β-Mn0.68600.68600.6860[27]
0.68760.68760.6876-24.132This work
Al-C-NbNb2AlChP8P63/mmcCr2AlC0.31050.31051.3890[28]
0.31090.31091.3920-61.168This work
Al-C-TaTa2AlChP8P63/mmcCr2AlC0.30750.30751.3830[28]
0.30900.30901.3962-56.071This work
Ta5Al3ChP16P63/mcmβ-Mn5Si30.52450.52450.7734[28]
0.53310.53310.7792-38.484This work
Al-C-VV2AlChP8P63/mmcCr2AlC0.29110.29111.3140[29]
-47.08±3.53[31]
0.28920.28921.3176-51.750This work
), ArticleFig(id=1321926676926287966, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=EN, label=Table 2, caption=

Thermodynamic parameters for the optimized Al-C-X(X=Mo,Nb,Ta,V) systems

, figureFileSmall=null, figureFileBig=null, tableContent=
SystemPhaseThermodynamic parameters a
Al-C-Mo

Mo3Al2C

(Mo)3(Al)2(C)

0GMo∶Al∶CMo3Al2C=-144792.62+3GMoSER+2GAlSER+GCSER
Al-C-Nb

Nb2AlC

(Nb)2(Al)(C)

0GNb∶Al∶CNb2AlC=-249672.37+15T+2GNbSER+GAlSER+GCSER
Al-C-Ta

Ta2AlC

(Ta)2(Al)(C)

0GTa∶Al∶CTa2AlC=-256000+515T-90.69Tln(T)

-0.009502T2+112791.75T-0.0000006148T2

Ta5Al3C

(Ta)5(Al)3(C)

0GTa∶Al∶CTa5Al3C=-346356.93+20T+5GTaSER+3GAlSER+GCSER
Al-C-V

V2AlC

(V)2(Al)(C)

0GV∶Al∶CV2AlC=-237000+515T-90.54Tln(T)

-0.01079T2+792349.45T-0.0000008552T3

), ArticleFig(id=1321926677047922783, tenantId=1146029695717560320, journalId=1220038251117760515, articleId=1321511462913290937, language=CN, label=表2, caption=

优化的Al-C-X (X=Mo,Nb,Ta,V)体系的热力学参数

, figureFileSmall=null, figureFileBig=null, tableContent=
SystemPhaseThermodynamic parameters a
Al-C-Mo

Mo3Al2C

(Mo)3(Al)2(C)

0GMo∶Al∶CMo3Al2C=-144792.62+3GMoSER+2GAlSER+GCSER
Al-C-Nb

Nb2AlC

(Nb)2(Al)(C)

0GNb∶Al∶CNb2AlC=-249672.37+15T+2GNbSER+GAlSER+GCSER
Al-C-Ta

Ta2AlC

(Ta)2(Al)(C)

0GTa∶Al∶CTa2AlC=-256000+515T-90.69Tln(T)

-0.009502T2+112791.75T-0.0000006148T2

Ta5Al3C

(Ta)5(Al)3(C)

0GTa∶Al∶CTa5Al3C=-346356.93+20T+5GTaSER+3GAlSER+GCSER
Al-C-V

V2AlC

(V)2(Al)(C)

0GV∶Al∶CV2AlC=-237000+515T-90.54Tln(T)

-0.01079T2+792349.45T-0.0000008552T3

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Al-C-X(X=Mo,Nb,Ta,V)的相图热力学计算
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石闯 , 夏新 , 张伟彬 , 王伟礼 , 韩桂芳 , 龚红宇 , 张景德
材料工程 | 研究论文 2025,53(12): 200-207
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材料工程 |研究论文 2025 , 53 (12) : 200 -207
Al-C-X(X=Mo,Nb,Ta,V)的相图热力学计算
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石闯, 夏新, 张伟彬 , 王伟礼, 韩桂芳, 龚红宇, 张景德
作者信息
  • 山东大学 材料液固结构演化与加工重点 实验室(教育部),济南 250061
通讯作者:
张伟彬(1985—),男,教授,博士,研究方向为硬质合金材料设计与产品研发,联系地址:山东省济南市历下区山东大学千佛山校区材料科学与工程学院(250061),E-mail:
Thermodynamic calculation of phase diagrams for Al-C-X(X=Mo,Nb,Ta,V)
Chuang SHI, Xin XIA, Weibin ZHANG , Weili WANG, Guifang HAN, Hongyu GONG, Jingde ZHANG
Affiliations
  • Key Laboratory for Liquid-Solid Structural Evolution and Processing of Materials (Ministry of Education),Shandong University,Jinan 250061,China
出版时间: 2025-12-20 doi: 10.11868/j.issn.1001-4381.2023.000668
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采用相图计算(calculation of phase diagrams, CALPHAD)耦合第一性原理计算对Al-C-X(X=Mo,Nb,Ta,V)体系进行了热力学研究。Al-C-Mo、Al-C-Nb和Al-C-V体系都只存在一个三元热力学稳定相,分别是Mo3Al2C、Nb2AlC和V2AlC。Al-C-Ta体系中的三元化合物为Ta5Al3C和Ta2AlC。通过第一性原理计算得到了这些化合物的生成焓,采用线性化合物模型描述其吉布斯自由能,最终由CALPHAD方法得到了一系列自洽的热力学参数。研究表明:优化得到的等温截面图和热力学数据与实验和计算结果均十分吻合。Al-C-X(X=Mo,Nb,Ta,V)体系的热力学参数能够帮助建立起析出强化黏结相的硬质合金数据库,指导设计具有优异性能的新型材料。

相图  /  热力学  /  相图计算  /  第一性原理计算

The Al-C-X(X=Mo,Nb,Ta,V) systems are studied by CALPHAD (calculation of phase diagrams) coupled with first-principles calculations. Two ternary phases,Ta5Al3C and Ta2AlC are identified in the Al-C-Ta system. All of the other three systems exist only one stable ternary phase, Mo3Al2C for Al-C-Mo, Nb2AlC for Al-C-Nb, and V2AlC for Al-C-V, respectively. The enthalpies of formation of these compounds are obtained by First-principles calculations, and their Gibbs free energies are presented by stoichiometric models. Finally, a series of self-consistent thermodynamic parameters are derived by CALPHAD method. The optimized isothermal sections and thermodynamic properties are in good agreement with experimental and computational results. The Al-C-X (X=Mo,Nb,Ta,V) systems assessed in this work can help to establish a thermodynamic database of hard alloys with precipitation strengthening bonding phases, which will be used to guide the design of new materials with excellent properties.

phase diagram  /  thermodynamics  /  CALPHAD  /  first-principles calculations
石闯, 夏新, 张伟彬, 王伟礼, 韩桂芳, 龚红宇, 张景德. Al-C-X(X=Mo,Nb,Ta,V)的相图热力学计算. 材料工程, 2025 , 53 (12) : 200 -207 . DOI: 10.11868/j.issn.1001-4381.2023.000668
Chuang SHI, Xin XIA, Weibin ZHANG, Weili WANG, Guifang HAN, Hongyu GONG, Jingde ZHANG. Thermodynamic calculation of phase diagrams for Al-C-X(X=Mo,Nb,Ta,V)[J]. Journal of Materials Engineering, 2025 , 53 (12) : 200 -207 . DOI: 10.11868/j.issn.1001-4381.2023.000668
传统WC-Co硬质合金是采用粉末冶金方法制备的复合材料,WC硬质颗粒赋予了合金较高的耐磨性和承受载荷的能力,而Co基黏结剂则赋予了合金良好的耐冲击性。由于硬质合金在强度、耐磨性、抗冲击韧性和热稳定性等方面的优良特性,被誉为“工业的牙齿”,广泛地用于切削加工、矿山开采、地质勘探、模具制造等工业领域[1]。伴随着国家先进制造业和重大装备制造的发展,硬质合金作为关键工业材料,市场需求巨大。与硬质相WC相比,Co基黏结剂在恶劣服役工况中自身性能不足,如优先磨损、高温氧化、耐腐蚀性差等,这已成为限制合金使用寿命的重要因素[2]。因此,想要制备高强韧、耐高温、抗腐蚀等性能优异的硬质合金材料,强化Co基黏结剂的研究是非常必要和迫切的。
在过去几十年里,强化黏结剂的有效途径是引入微量元素(如Cr、Ni、Mo等)通过固溶强化一定程度上强化黏结剂的耐磨性、耐蚀性和高温性能[3]。近年来,借鉴新型γ/γ′两相组织Co基高温合金[4-5],在硬质合金Co-Ni3Al复合黏结剂中沉淀析出有序结构的纳米增强相,可以使得合金兼具良好的硬度和韧性,并大幅提升抗氧化性和耐腐蚀性[6-9]。在此基础上,有研究者关注于合金黏结剂中析出相的结构调控。例如,Biurrun等[10]研究了WC-Ni-Co-Cr-Ti-Al硬质合金中不同元素含量添加及时效处理对γ′析出相和材料性能的影响。黄公治[11]研究了AlN添加量及时效时间对WC-13.2Co-15.3Ni-1.5Cr3C2合金γ′析出相尺寸及力学性能的影响。
目前,有序析出相强化硬质合金黏结剂的研究体系较少且缺乏系统基础性研究,合金各方面的性能仍有大幅提升空间。在Co基高温合金中,Mo、Nb、Ta、V均为γ'相强稳定元素,能够提高γ'相的固溶温度与体积分数,进而影响合金的高温性能[12]。另外,在传统WC-Co硬质合金中添加Mo2C、NbC、TaC、VC等碳化物晶粒抑制剂也对材料性能有有益作用[13]。综上所述,在有序析出相强化硬质合金黏结剂体系中,引入这些元素进一步开发和设计有望获得高强韧、耐高温、抗腐蚀等性能优异的硬质合金材料。
多元合金烧结过程存在复杂的热力学现象,不同含量元素的复合添加会对形成的显微组织产生明显的影响。建立1套准确的热力学数据库,有助于科学设计合金成分和工艺参数,加速有序析出相强化硬质合金材料的研发[14]。中南大学杜勇教授团队[15]对WC-Co-Ni-Al体系相图开展了系统的研究工作,并构建了完整的热力学数据库。引入Mo、Nb、Ta、V等元素后,在此数据库里增加的相关多元体系的报道还不够全面,本工作对涉及的Al-C-Mo、Al-C-Nb、Al-C-Ta和Al-C-V体系进行了相图热力学研究。Al-C-X(X=Mo,Nb,Ta,V)体系组成较为简单,且相图研究结果的争议较小,通过有限的理论计算即能够得到可靠的三元热力学数据库。在工作中体系的三元相均简化为线性化合物模型,并用第一性原理计算得到了它们的生成焓。然后利用CALPHAD方法优化得到了能够准确描述理论计算和实验数据的热力学模型参数。计算的Al-C-X(X=Mo,Nb,Ta,V)体系参数能够帮助建立起完备的硬质合金热力学数据库,指导新型Co基黏结剂硬质合金的设计。
CALPHAD是材料设计中十分高效的工具,可以通过对体系组分吉布斯自由能的建模预测所感兴趣的成分和温度下的相图信息[16]。模型和模型参数取决于晶体结构,评估的相平衡数据、热力学性质数据等。
文中沿用了Dinsdale编纂的欧洲标准热力学数据库[17]中的参数对纯组元Al、C、Mo、Nb、Ta和V的吉布斯自由能进行描述。二元体系数据库Al-C、Al-Mo、Al-Nb、Al-Ta、Al-V、C-Mo、C-Nb、C-Ta、C-V采用文献[18-26]中的模型和参数。
在Al-C-Mo体系中,唯一被报道的三元相是Mo3Al2C[27]。Al-C-Nb、Al-C-Ta和Al-C-V体系中都存在典型的MAX结构相(H-phase),分别是Nb2AlC[28]、Ta2AlC[28]和V2AlC[29]。另外在Al-C-Ta体系中,β-Mn5Si3结构的化合物Ta5Al3C在相对较小的温度范围内也是稳定的[28]。没有实验数据表明这些三元化合物存在明显的固溶度,因此体系的三元化合物的吉布斯自由能均由线性化合物模型描述。在化合物Ta2AlC和V2AlC的热力学建模时,考虑了文献[30-31]中给出的由室温至高温的热容数据。以V2AlC为例,其吉布斯自由能Gm可以用1个与温度相关的多项式表示:
0GmV2AlC=a+bT+cTln(T)+dT2+eT-1+fT3
式中:Gm为吉布斯自由能;T为绝对温度;a、b、c、d、e、f是本工作中待优化的参数。
对化合物Ta5Al3C、Mo3Al2C和Nb2AlC使用了更为简单的线性模型,三者的热容值由Neumann-Kopp 规则[32]确定。以Mo3Al2C为例,其吉布斯自由能表达形式如下:
0GmMo3Al2C=A+BT+xMo⋅GMoSER+xAl⋅GAlSER+xC⋅GCSER
式中:xMo、xAl、xC分别代表Mo、Al、C在化合物Mo3Al2C中占据的原子分数;GMoSER、GAlSER、GCSER为Mo、Al、C在各自SER状态下的吉布斯自由能函数;A和B是在本工作中待优化的参数。
上述两式中参数的确定都是在Thermo-calc程序包中的PARROT模块[33]完成的。
第一性原理是迭代求解微观粒子方程,获取体系基态性质的计算方法[14]。在材料设计中常用来计算结构稳定性和力、热、电、光、磁学等性质。
第一性原理计算是在基于密度泛函理论的vienna ab initio simulation package(VASP)软件包[34]中完成的。计算的交换关联能采用广义梯度近似泛函的Perdew-Burke-Ernzerhof(PBE)[35]形式,电子间的相互作用用投影缀加平面波[36]描述。平面波截断能设置为520 eV。在布里渊区以Monkhorst-Pack方法[37]对K点取值。Mo3Al2C、Nb2AlC、Ta2AlC、Ta5Al3C、V2AlC的K点分别为3×3×3、5×5×3、7×7×3、4×4×6、5×5×3。结构优化采取完全弛豫确定晶胞和原子坐标,电子自洽计算精度为1×10-4 eV,原子弛豫收敛标准为-0.005 eV·nm-1。结构稳定后静态计算以提高能量的计算精度。
第一性原理计算得到的化合物生成焓是CALPHAD所拟合吉布斯自由能函数初始值的可靠输入。有研究人员通过第一性原理得到的生成焓数据结合CALPHAD,计算了合成温度下未知化合物的稳定性,指导后续的实验设计[38]。在CALPHAD的许多案例中,也可以直接将第一性原理计算得到的生成焓固定为能量函数的常数部分,即式(2)中的A值[39-40]。在0 K下,第一性原理计算的V2AlC生成焓ΔHfV2AlC可用如下方程表示:
ΔHfV2AlC=EV2AlC-NV⋅EV-NAl⋅EAl-NC⋅ECNV+NAl+NC
式中:EV2AlC为计算的V2AlC化合物总能;NV、NAl、NC分别为V2AlC晶胞中V、Al、C的原子数;EV、EAl、EC分别为基态原子V、Al、C的总能。
首先采用第一性原理对化合物Nb2AlC、V2AlC、Ta2AlC、Ta5Al3C和Mo3Al2C进行了晶体结构的优化,并计算其标准生成焓。这些化合物的晶体信息和生成焓数据整理在表1[27-29,31]中。对比可知,计算的化合物的晶格参数与实验测定的结果差别很小,表明第一性原理的结果是可靠的。其中,Agne等[31]用求解化学平衡的方法给出了化合物V2AlC在25 ℃的生成焓,其值的不确定性源于选取的参考态能量。第一性原理计算的生成焓结果负值稍大。
由第一性原理计算的生成焓和文献中的等温截面图、部分化合物的热力学数据,优化得到了三元线性化合物的热力学参数。优化的模型参数列在表2中。图1给出了由热力学参数计算得到的化合物生成焓。Mo3Al2C、Nb2AlC、Ta5Al3C、Ta2AlC、V2AlC的生成焓分别为-24.132、-62.414、-38.484、-56.282、-50.580 kJ∙mol·atom-1,均能与第一性原理的计算结果匹配。结合文献评估结果,分别对Al-C-Mo、Al-C-Nb、Al-C-Ta和Al-C-V 4个体系的相图计算进行讨论。
Jeitschko等[27]熔炼了不同成分的Al-C-Mo合金,通过X射线衍射(XRD)和金相观测研究了该体系1450 ℃和1000 ℃的相关。体系中仅能检测到一个三元化合物Mo3Al2C,Mo的含量为47~51%(原子分数,下同),在1450 ℃和1000 ℃都稳定存在。Reith等[41]理论计算证明碳空位浓度约为2%的Mo3Al2C相仍能保持热力学稳定性。该化合物的固溶范围很小,故可简化为线性化合物模型对其进行描述。在参数优化过程中,用第一性原理的生成焓确定A值,计算已经与实验符合的很好,因此,没有引入更多的参数。
文中计算的Al-C-Mo体系1000 ℃和1450 ℃的等温截面分别如图2(a)和图2(b)所示。2个等温截面下三元化合物Mo3Al2C都参与形成了4个三相区:Mo3Al2C+Mo2C+Mo3Al,Mo3Al2C+Mo2C+Al4C3,Mo3Al2C+Mo2C+Al4C3+C,Mo3Al2C+Mo3Al+Mo3Al8。在Mo含量较高时,Mo3Al2C的竞争相为Mo2C和Mo3Al,其不能实现与BCC相(Mo固溶体)的平衡。Karki等[42]曾用电弧熔炼的方法制备了Mo3Al2C,XRD结果显示其杂相除Mo3Al8外,还有Mo。根据计算的相图,该结果可能是熔炼不均匀所致。在1000 ℃时,相比于1450 ℃,Mo-C体系[23]增加了MoC相,Al-Mo体系[19]中Mo3Al8部分分解为Mo3Al和Mo4Al。Mo3Al2C参与形成的平衡相区基本没有变化。本文计算的2个等温截面均与实验结果符合。
Schuster等[28]通过XRD测定了Al-C-Nb体系在1000 ℃和700 ℃的等温截面图。三元化合物Nb2AlC存在极小的均质范围,在700~1000 ℃之间都稳定存在。该体系二元相中不存在明显的第三组元的溶解度。在优化过程中,Nb2AlC的线性化合物模型参数是根据第一性原理计算的生成焓以及两个等温截面图确定的。
计算的Al-C-Nb体系700 ℃和1000 ℃的等温截面分别如图3(a)和图3(b)所示,2个温度下的体系相关系基本一致。在此温度区间二元体系的稳定相有NbAl3、σ(Nb2Al)、NbAl3、Nb2C、NbC、Al4C3。Nb2AlC能够和其中除Al4C3之外的化合物形成平衡。在1000 ℃,Schuster等根据粉末合成过程发生的化学反应推测存在NbC和Al(Liquid)的两相平衡。根据相图计算结果,零变量反应NbC+Al(Liquid)=NbAl3+Al4C3的温度约为1288.2 ℃。因此低于该温度NbC和Al(Liquid)不能实现平衡,富Al角为Al4C3-NbC-NbAl3和Al4C3-Al-NbAl3 2个三相区。计算的相图与实验相图基本一致。
Schuster等[28]通过XRD测定了Al-C-Ta体系在700 ℃和1000 ℃的等温截面图。体系存在2个三元碳化物,Ta2AlC和Ta5Al3C。Ta5Al3C只在1000 ℃的截面图中出现,中低温下发生分解。根据文献[21],低于1000 ℃时Al-Ta体系中的稳定相为TaAl3、TaAl(φ)和Ta2Al(σ),因此本工作计算中没有考虑Schuster等检测到的计量成分为Ta2Al3的化合物。Hu等[30]用热性能分析仪测定了Ta2AlC从室温至高温的热容。Drulis等[43]用绝热量热器测定了低温下(3~260 K)Ta2AlC的热容值。两者实验数据的一致性较差,本次计算时只考虑了Hu等测得的热容数据。在优化过程中,由热容和第一性原理计算的生成焓初步确定了Ta2AlC和Ta5Al3C的模型参数,后根据700 ℃和1000 ℃ 2个等温截面对参数做了进一步调整。
计算的Ta2AlC的热容结合文献测定的数据如图4所示。对比可知计算结果与实验一致性很好。Al-C-Ta体系的700 ℃和1000 ℃等温截面分别如图5(a)和图5(b)所示。在2个等温截面图中三元碳化物Ta2AlC都稳定存在,其和TaC、Ta2C、TaAl3形成了一些三相区。Schuster等没有考虑φ相的存在,计算结果显示φ、σ和Ta2C也形成了1个三相区。在1000 ℃,Schuster等检测到Ta5Al3C和Ta2Al3参与形成了2个三相区,分别是Ta5Al3C+Ta2Al3+TaAl3和Ta5Al3C+Ta2Al3+σ。将对应Ta2Al3成分下的化合物视为亚稳相,计算的等温截面只存在Ta5Al3C、φ和TaAl3的三相平衡。需要说明的是,若要得到Ta5Al3C和σ之间的平衡,前者将与Ta2AlC等化合物形成额外的相区。与Al-C-Cr三元系[44]类似,在体系缺乏科学自洽实验结论的情况下,在计算过程中对热力学参数进行了不同范围的调整。最终采用了能够协调第一性原理计算与实验结果的热力学参数。除Ta5Al3C外,两个等温截面的另一个明显区别是在1000 ℃,TaC和Al(Liquid)形成了两相平衡。计算的相图与实验相图基本一致。
Schuster等[29]测定了Al-C-V体系在1000 ℃的等温截面图。体系中只存在1个稳定的三元化合物V2AlC。XRD测试结果表明体系中化合物均不存在明显的溶解度。Agne等[45]通过原位合成的方法制得了Al-V2AlC复合材料,利用XRD、扫描电子显微镜(SEM)、差示扫描量热法(DSC)等研究了其在800~1000 ℃的稳定性。Agne等[31]通过第一性原理计算得到了V2AlC的热容,进而通过化学平衡计算了生成焓、自由能等。依赖于CALPHAD方法得到自洽的热力学参数,与Agne等[31]化学平衡计算过程选择的参考态不同。因此在优化时,主要以Agne等第一性原理方法计算的热容、计算的生成焓以及Al-C-V体系在1000 ℃和800 ℃的相关系来确定参数取值。
计算的V2AlC的热容结合文献给出的数据如图6所示,对比可知计算结果与文献符合。Al-C-V体系的800 ℃和1000 ℃等温截面分别如图7(a)和图7(b)所示。2个温度下V2AlC都显示了非常高的热力学稳定性,与体系中所有的二元化合物都存在平衡。在800 ℃,V2AlC、Al(Liquid)分别和Al3V、Al4C3形成了2个三相区。而在1000 ℃,V2AlC与Al(Liquid)形成了两相平衡。根据DSC的测定结果,零变量反应V2AlC+Al(Liquid)=Al4C3+Al3V的温度约为938 ℃[41]。该工作计算的反应温度为938.3 ℃,与实验一致性很好。
(1)在Co基高温合金中的研究中,Mo、Nb、Ta、V等元素显示了其在析出强化材料中的良好应用前景。本文所研究的Al-C-X(X=Mo,Nb,Ta,V)是有序相析出强化硬质合金引入这些元素后涉及到的重要子体系。
(2)采用第一性原理计算了Mo3Al2C、Nb2AlC、Ta2AlC、Ta5Al3C和V2AlC的晶格参数与生成焓,这些化合物的吉布斯自由能均由线性化合物模型描述。
(3)结合理论计算结果和实验数据,优化得到了一系列自洽的CALPHAD热力学参数。计算得到的Al-C-Mo、Al-C-Nb、Al-C-Ta和Al-C-V体系等温截面图与实验结论基本一致。
(4)本工作最终能够帮助建立起完善的硬质合金数据库,掌握多元体系的热力学信息,科学指导硬质合金的成分工艺设计和性能预测,加速硬质合金新型黏结剂体系的开发。
  • 国家重点研发计划(2023YFB3712600)
  • 国家自然科学基金(52171009)
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doi: 10.11868/j.issn.1001-4381.2023.000668
  • 接收时间:2023-10-08
  • 首发时间:2026-10-26
  • 出版时间:2025-12-20
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  • 收稿日期:2023-10-08
  • 录用日期:2024-09-19
基金
国家重点研发计划(2023YFB3712600)
国家自然科学基金(52171009)
作者信息
    山东大学 材料液固结构演化与加工重点 实验室(教育部),济南 250061

通讯作者:

张伟彬(1985—),男,教授,博士,研究方向为硬质合金材料设计与产品研发,联系地址:山东省济南市历下区山东大学千佛山校区材料科学与工程学院(250061),E-mail:
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https://castjournals.cast.org.cn/joweb/clgc/CN/10.11868/j.issn.1001-4381.2023.000668
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2种不同金属材料的力学参数
科
Family
属数
Number of
genus
种数
Number of
species
占总种数比例
Percentage of
total species (%)
属
Genus
种数
Number of
species
占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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