Gibbs energy-composition plots as a tool for high-entropy alloy design

In the present study, an approach based on binary Gibbs energy-composition (G-x) plots is used for understanding the phase constitution in high-entropy alloys (HEAs). Equimolar HEAs CoCrMnNi, CoCrCuMnNi and AlCoCrMnNi were made using vacuum arc melting and heat treated for 24 h at 1000 °C. XRD and S...

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Veröffentlicht in:Journal of alloys and compounds 2018-11, Vol.768, p.358-367
Hauptverfasser: Guruvidyathri, K., Murty, B.S., Yeh, J.W., Hari Kumar, K.C.
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creator Guruvidyathri, K.
Murty, B.S.
Yeh, J.W.
Hari Kumar, K.C.
description In the present study, an approach based on binary Gibbs energy-composition (G-x) plots is used for understanding the phase constitution in high-entropy alloys (HEAs). Equimolar HEAs CoCrMnNi, CoCrCuMnNi and AlCoCrMnNi were made using vacuum arc melting and heat treated for 24 h at 1000 °C. XRD and SEM were used for the characterization of constituent phases. A method based on the G-x plots of binary sub-systems was devised for the interpretation of the constituent phases in these alloys and a few other HEAs reported in the literature, namely CoCrFeMnNi and CoCuFeMnNi. The competition between phases and demixing tendencies were correlated with the G-x plots. These plots revealed that in CoCrMnNi and CoCrFeMnNi, tendency for formation of intermetallic phases and demixing were absent. This correlated well with their single-phase disordered FCC (A1) microstructure. On the other hand, the CoCrCuMnNi alloy had a duplex microstructure consisting of two FCC phases that can be attributed to the strong demixing tendency for FCC phase in the Cr-Cu system. The microstructure of the CoCuFeMnNi consisted only single FCC phase. Though, two of the constituent binaries showed tendency for demixing of this FCC phase, it is not strong enough to cause immiscibility. The AlCoCrMnNi alloy gave a duplex microstructure of an ordered (B2) and a disordered (A2) BCC phase. G-x plots showed that the competition from B2 phase in binaries is so strong that its formation inevitably occurred in this HEA. Such crucial insights into how strongly the thermodynamics of the binary sub-systems control the phase constitution in HEAs are offered by the present approach. Although the results can in principle be interpreted using comprehensive Calphad calculations, one requires reliable multicomponent Gibbs energy databases to do so. The approach presented here is rather simple, as it requires only Gibbs energy functions of relevant phases of the constituent binary systems. [Display omitted] •Binary Gibbs energy profoundly influences HEA phase constitution.•First simple HEA design approach is proposed that relies binary Gibbs energy data.•Binary systems with smaller demixing tendency do not cause demixing in HEA.•Weekly competing intermetallic phases in binary systems do not appear in HEA.
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Equimolar HEAs CoCrMnNi, CoCrCuMnNi and AlCoCrMnNi were made using vacuum arc melting and heat treated for 24 h at 1000 °C. XRD and SEM were used for the characterization of constituent phases. A method based on the G-x plots of binary sub-systems was devised for the interpretation of the constituent phases in these alloys and a few other HEAs reported in the literature, namely CoCrFeMnNi and CoCuFeMnNi. The competition between phases and demixing tendencies were correlated with the G-x plots. These plots revealed that in CoCrMnNi and CoCrFeMnNi, tendency for formation of intermetallic phases and demixing were absent. This correlated well with their single-phase disordered FCC (A1) microstructure. On the other hand, the CoCrCuMnNi alloy had a duplex microstructure consisting of two FCC phases that can be attributed to the strong demixing tendency for FCC phase in the Cr-Cu system. The microstructure of the CoCuFeMnNi consisted only single FCC phase. Though, two of the constituent binaries showed tendency for demixing of this FCC phase, it is not strong enough to cause immiscibility. The AlCoCrMnNi alloy gave a duplex microstructure of an ordered (B2) and a disordered (A2) BCC phase. G-x plots showed that the competition from B2 phase in binaries is so strong that its formation inevitably occurred in this HEA. Such crucial insights into how strongly the thermodynamics of the binary sub-systems control the phase constitution in HEAs are offered by the present approach. Although the results can in principle be interpreted using comprehensive Calphad calculations, one requires reliable multicomponent Gibbs energy databases to do so. The approach presented here is rather simple, as it requires only Gibbs energy functions of relevant phases of the constituent binary systems. [Display omitted] •Binary Gibbs energy profoundly influences HEA phase constitution.•First simple HEA design approach is proposed that relies binary Gibbs energy data.•Binary systems with smaller demixing tendency do not cause demixing in HEA.•Weekly competing intermetallic phases in binary systems do not appear in HEA.</description><identifier>ISSN: 0925-8388</identifier><identifier>EISSN: 1873-4669</identifier><identifier>DOI: 10.1016/j.jallcom.2018.07.264</identifier><language>eng</language><publisher>Lausanne: Elsevier B.V</publisher><subject>Alloy design ; Alloys ; Arc heating ; Binary systems ; CALPHAD ; Chromium ; Competition ; Composition ; Computer simulation ; Constituents ; Constitution ; Copper ; Demixing ; Electric arc melting ; Gibbs energy ; Heat treatment ; High entropy alloys ; Intermetallic phases ; Microstructure ; Miscibility ; Phase transitions ; Scanning electron microscopy ; Thermodynamics ; Vacuum arc melting</subject><ispartof>Journal of alloys and compounds, 2018-11, Vol.768, p.358-367</ispartof><rights>2018 Elsevier B.V.</rights><rights>Copyright Elsevier BV Nov 5, 2018</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c403t-d54f753289460153c07dcdc908a15cf43c8bfedf0af0a22470c9030306e3b57a3</citedby><cites>FETCH-LOGICAL-c403t-d54f753289460153c07dcdc908a15cf43c8bfedf0af0a22470c9030306e3b57a3</cites><orcidid>0000-0002-8335-7931</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0925838818327658$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65306</link.rule.ids></links><search><creatorcontrib>Guruvidyathri, K.</creatorcontrib><creatorcontrib>Murty, B.S.</creatorcontrib><creatorcontrib>Yeh, J.W.</creatorcontrib><creatorcontrib>Hari Kumar, K.C.</creatorcontrib><title>Gibbs energy-composition plots as a tool for high-entropy alloy design</title><title>Journal of alloys and compounds</title><description>In the present study, an approach based on binary Gibbs energy-composition (G-x) plots is used for understanding the phase constitution in high-entropy alloys (HEAs). Equimolar HEAs CoCrMnNi, CoCrCuMnNi and AlCoCrMnNi were made using vacuum arc melting and heat treated for 24 h at 1000 °C. XRD and SEM were used for the characterization of constituent phases. A method based on the G-x plots of binary sub-systems was devised for the interpretation of the constituent phases in these alloys and a few other HEAs reported in the literature, namely CoCrFeMnNi and CoCuFeMnNi. The competition between phases and demixing tendencies were correlated with the G-x plots. These plots revealed that in CoCrMnNi and CoCrFeMnNi, tendency for formation of intermetallic phases and demixing were absent. This correlated well with their single-phase disordered FCC (A1) microstructure. On the other hand, the CoCrCuMnNi alloy had a duplex microstructure consisting of two FCC phases that can be attributed to the strong demixing tendency for FCC phase in the Cr-Cu system. The microstructure of the CoCuFeMnNi consisted only single FCC phase. Though, two of the constituent binaries showed tendency for demixing of this FCC phase, it is not strong enough to cause immiscibility. The AlCoCrMnNi alloy gave a duplex microstructure of an ordered (B2) and a disordered (A2) BCC phase. G-x plots showed that the competition from B2 phase in binaries is so strong that its formation inevitably occurred in this HEA. Such crucial insights into how strongly the thermodynamics of the binary sub-systems control the phase constitution in HEAs are offered by the present approach. Although the results can in principle be interpreted using comprehensive Calphad calculations, one requires reliable multicomponent Gibbs energy databases to do so. The approach presented here is rather simple, as it requires only Gibbs energy functions of relevant phases of the constituent binary systems. [Display omitted] •Binary Gibbs energy profoundly influences HEA phase constitution.•First simple HEA design approach is proposed that relies binary Gibbs energy data.•Binary systems with smaller demixing tendency do not cause demixing in HEA.•Weekly competing intermetallic phases in binary systems do not appear in HEA.</description><subject>Alloy design</subject><subject>Alloys</subject><subject>Arc heating</subject><subject>Binary systems</subject><subject>CALPHAD</subject><subject>Chromium</subject><subject>Competition</subject><subject>Composition</subject><subject>Computer simulation</subject><subject>Constituents</subject><subject>Constitution</subject><subject>Copper</subject><subject>Demixing</subject><subject>Electric arc melting</subject><subject>Gibbs energy</subject><subject>Heat treatment</subject><subject>High entropy alloys</subject><subject>Intermetallic phases</subject><subject>Microstructure</subject><subject>Miscibility</subject><subject>Phase transitions</subject><subject>Scanning electron microscopy</subject><subject>Thermodynamics</subject><subject>Vacuum arc melting</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNqFUF1LwzAUDaLgnP4EIeBz681Xkz6JDDeFgS_6HNo03VK6piad0H9vxvYu98B9uOeDexB6JJATIMVzl3dV3xt_yCkQlYPMacGv0IIoyTJeFOU1WkBJRaaYUrfoLsYOAEjJyAKtN66uI7aDDbs5Sx6jj25yfsBj76eIqwQ8ed_j1ge8d7t9Zocp-HHGKdPPuLHR7YZ7dNNWfbQPl71E3-u3r9V7tv3cfKxet5nhwKasEbyVglFV8gKIYAZkYxpTgqqIMC1nRtWtbVqoEijlEtKNpSksq4Ws2BI9nX3H4H-ONk6688cwpEhNCS0FLbkkiSXOLBN8jMG2egzuUIVZE9CnynSnL5XpU2UapE6VJd3LWWfTC7_OBh2Ns4OxjQvWTLrx7h-HPy1zdwo</recordid><startdate>20181105</startdate><enddate>20181105</enddate><creator>Guruvidyathri, K.</creator><creator>Murty, B.S.</creator><creator>Yeh, J.W.</creator><creator>Hari Kumar, K.C.</creator><general>Elsevier B.V</general><general>Elsevier BV</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><orcidid>https://orcid.org/0000-0002-8335-7931</orcidid></search><sort><creationdate>20181105</creationdate><title>Gibbs energy-composition plots as a tool for high-entropy alloy design</title><author>Guruvidyathri, K. ; Murty, B.S. ; Yeh, J.W. ; Hari Kumar, K.C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c403t-d54f753289460153c07dcdc908a15cf43c8bfedf0af0a22470c9030306e3b57a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Alloy design</topic><topic>Alloys</topic><topic>Arc heating</topic><topic>Binary systems</topic><topic>CALPHAD</topic><topic>Chromium</topic><topic>Competition</topic><topic>Composition</topic><topic>Computer simulation</topic><topic>Constituents</topic><topic>Constitution</topic><topic>Copper</topic><topic>Demixing</topic><topic>Electric arc melting</topic><topic>Gibbs energy</topic><topic>Heat treatment</topic><topic>High entropy alloys</topic><topic>Intermetallic phases</topic><topic>Microstructure</topic><topic>Miscibility</topic><topic>Phase transitions</topic><topic>Scanning electron microscopy</topic><topic>Thermodynamics</topic><topic>Vacuum arc melting</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guruvidyathri, K.</creatorcontrib><creatorcontrib>Murty, B.S.</creatorcontrib><creatorcontrib>Yeh, J.W.</creatorcontrib><creatorcontrib>Hari Kumar, K.C.</creatorcontrib><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of alloys and compounds</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guruvidyathri, K.</au><au>Murty, B.S.</au><au>Yeh, J.W.</au><au>Hari Kumar, K.C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Gibbs energy-composition plots as a tool for high-entropy alloy design</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2018-11-05</date><risdate>2018</risdate><volume>768</volume><spage>358</spage><epage>367</epage><pages>358-367</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>In the present study, an approach based on binary Gibbs energy-composition (G-x) plots is used for understanding the phase constitution in high-entropy alloys (HEAs). Equimolar HEAs CoCrMnNi, CoCrCuMnNi and AlCoCrMnNi were made using vacuum arc melting and heat treated for 24 h at 1000 °C. XRD and SEM were used for the characterization of constituent phases. A method based on the G-x plots of binary sub-systems was devised for the interpretation of the constituent phases in these alloys and a few other HEAs reported in the literature, namely CoCrFeMnNi and CoCuFeMnNi. The competition between phases and demixing tendencies were correlated with the G-x plots. These plots revealed that in CoCrMnNi and CoCrFeMnNi, tendency for formation of intermetallic phases and demixing were absent. This correlated well with their single-phase disordered FCC (A1) microstructure. On the other hand, the CoCrCuMnNi alloy had a duplex microstructure consisting of two FCC phases that can be attributed to the strong demixing tendency for FCC phase in the Cr-Cu system. The microstructure of the CoCuFeMnNi consisted only single FCC phase. Though, two of the constituent binaries showed tendency for demixing of this FCC phase, it is not strong enough to cause immiscibility. The AlCoCrMnNi alloy gave a duplex microstructure of an ordered (B2) and a disordered (A2) BCC phase. G-x plots showed that the competition from B2 phase in binaries is so strong that its formation inevitably occurred in this HEA. Such crucial insights into how strongly the thermodynamics of the binary sub-systems control the phase constitution in HEAs are offered by the present approach. Although the results can in principle be interpreted using comprehensive Calphad calculations, one requires reliable multicomponent Gibbs energy databases to do so. The approach presented here is rather simple, as it requires only Gibbs energy functions of relevant phases of the constituent binary systems. [Display omitted] •Binary Gibbs energy profoundly influences HEA phase constitution.•First simple HEA design approach is proposed that relies binary Gibbs energy data.•Binary systems with smaller demixing tendency do not cause demixing in HEA.•Weekly competing intermetallic phases in binary systems do not appear in HEA.</abstract><cop>Lausanne</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jallcom.2018.07.264</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-8335-7931</orcidid></addata></record>
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subjects Alloy design
Alloys
Arc heating
Binary systems
CALPHAD
Chromium
Competition
Composition
Computer simulation
Constituents
Constitution
Copper
Demixing
Electric arc melting
Gibbs energy
Heat treatment
High entropy alloys
Intermetallic phases
Microstructure
Miscibility
Phase transitions
Scanning electron microscopy
Thermodynamics
Vacuum arc melting
title Gibbs energy-composition plots as a tool for high-entropy alloy design
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