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The miscibility gap between the rock salt and wurtzite phases in the MgO–ZnO binary system to 3.5 GPa
At ambient pressure, MgO crystallizes in the rock salt (B1) structure, whereas ZnO crystallizes in the wurtzite structure (B4). The asymmetric miscibility gap between these two structures in the MgO–ZnO binary system narrows with increasing pressure, terminating at the wurtzite-to-rock-salt phase tr...
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Published in: | European journal of mineralogy (Stuttgart) 2023-11, Vol.35 (6), p.1051-1071 |
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description | At ambient pressure, MgO crystallizes in the rock salt (B1) structure, whereas ZnO crystallizes in the wurtzite structure (B4). The asymmetric miscibility gap between these two structures in the MgO–ZnO binary system narrows with increasing pressure, terminating at the wurtzite-to-rock-salt phase transition in pure ZnO, which occurs at approximately 5 GPa at 1000 ∘C. Despite their essential simplicity, the pressure–temperature–composition (P–T–X) relations in the MgO–ZnO binary system have been sparsely studied experimentally, with disparate results that are inconsistent with available thermodynamic data. Here we report the experimental determination of the P–T–X relations of the miscibility gap from 940 to 1500 ∘C and 0 to 3.5 GPa, which we combine with calorimetric and equation-of-state data from the literature and on the transition in endmember ZnO, to build a thermodynamic model that resolves many of the inconsistencies. The model treats the rock salt phase as an ideal solution (no excess Gibbs free energy of mixing), while in the wurtzite phase the MgO component follows Henry's law and the ZnO component Raoult's law in the range of compositions accessed experimentally. However, there is an inconsistency between the partial molar volume of wurtzite-structured MgO deduced from this model and that inferred from lattice parameter measurements by X-ray diffraction in the quenched samples. This discrepancy may be caused by unquenchable disordering of some significant fraction of the substituting Mg2+ into normally vacant octahedral interstices of the wurtzite structure. |
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The asymmetric miscibility gap between these two structures in the MgO–ZnO binary system narrows with increasing pressure, terminating at the wurtzite-to-rock-salt phase transition in pure ZnO, which occurs at approximately 5 GPa at 1000 ∘C. Despite their essential simplicity, the pressure–temperature–composition (P–T–X) relations in the MgO–ZnO binary system have been sparsely studied experimentally, with disparate results that are inconsistent with available thermodynamic data. Here we report the experimental determination of the P–T–X relations of the miscibility gap from 940 to 1500 ∘C and 0 to 3.5 GPa, which we combine with calorimetric and equation-of-state data from the literature and on the transition in endmember ZnO, to build a thermodynamic model that resolves many of the inconsistencies. The model treats the rock salt phase as an ideal solution (no excess Gibbs free energy of mixing), while in the wurtzite phase the MgO component follows Henry's law and the ZnO component Raoult's law in the range of compositions accessed experimentally. However, there is an inconsistency between the partial molar volume of wurtzite-structured MgO deduced from this model and that inferred from lattice parameter measurements by X-ray diffraction in the quenched samples. This discrepancy may be caused by unquenchable disordering of some significant fraction of the substituting Mg2+ into normally vacant octahedral interstices of the wurtzite structure.</description><identifier>ISSN: 1617-4011</identifier><identifier>ISSN: 0935-1221</identifier><identifier>EISSN: 1617-4011</identifier><identifier>DOI: 10.5194/ejm-35-1051-2023</identifier><language>eng</language><publisher>Göttingen: Copernicus GmbH</publisher><subject>Analysis ; Binary system ; Chemical properties ; Composition ; Equilibrium ; Experiments ; Gibbs free energy ; Henrys law ; Interstices ; Magnesium compounds ; Magnesium oxide ; Miscibility ; Molar volume ; Phase transitions ; Pressure ; Raoults law ; Rock-salt ; Rocks ; Salt ; Salts ; Solid solutions ; Solubility ; Temperature ; Thermodynamic models ; Thermodynamics ; Wurtzite ; X-ray diffraction ; Zinc oxide</subject><ispartof>European journal of mineralogy (Stuttgart), 2023-11, Vol.35 (6), p.1051-1071</ispartof><rights>COPYRIGHT 2023 Copernicus GmbH</rights><rights>2023. 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The asymmetric miscibility gap between these two structures in the MgO–ZnO binary system narrows with increasing pressure, terminating at the wurtzite-to-rock-salt phase transition in pure ZnO, which occurs at approximately 5 GPa at 1000 ∘C. Despite their essential simplicity, the pressure–temperature–composition (P–T–X) relations in the MgO–ZnO binary system have been sparsely studied experimentally, with disparate results that are inconsistent with available thermodynamic data. Here we report the experimental determination of the P–T–X relations of the miscibility gap from 940 to 1500 ∘C and 0 to 3.5 GPa, which we combine with calorimetric and equation-of-state data from the literature and on the transition in endmember ZnO, to build a thermodynamic model that resolves many of the inconsistencies. The model treats the rock salt phase as an ideal solution (no excess Gibbs free energy of mixing), while in the wurtzite phase the MgO component follows Henry's law and the ZnO component Raoult's law in the range of compositions accessed experimentally. However, there is an inconsistency between the partial molar volume of wurtzite-structured MgO deduced from this model and that inferred from lattice parameter measurements by X-ray diffraction in the quenched samples. This discrepancy may be caused by unquenchable disordering of some significant fraction of the substituting Mg2+ into normally vacant octahedral interstices of the wurtzite structure.</description><subject>Analysis</subject><subject>Binary system</subject><subject>Chemical properties</subject><subject>Composition</subject><subject>Equilibrium</subject><subject>Experiments</subject><subject>Gibbs free energy</subject><subject>Henrys law</subject><subject>Interstices</subject><subject>Magnesium compounds</subject><subject>Magnesium oxide</subject><subject>Miscibility</subject><subject>Molar volume</subject><subject>Phase transitions</subject><subject>Pressure</subject><subject>Raoults law</subject><subject>Rock-salt</subject><subject>Rocks</subject><subject>Salt</subject><subject>Salts</subject><subject>Solid solutions</subject><subject>Solubility</subject><subject>Temperature</subject><subject>Thermodynamic models</subject><subject>Thermodynamics</subject><subject>Wurtzite</subject><subject>X-ray diffraction</subject><subject>Zinc oxide</subject><issn>1617-4011</issn><issn>0935-1221</issn><issn>1617-4011</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><sourceid>DOA</sourceid><recordid>eNptkT1vFDEQhlcIJEKgp7REvYe9ttd2GUUQIgUdRWhorFnv-OLjdn3YPkVHlZY6_zC_JD4O8SEhW7I188yrmXmb5jWjC8mMeIvrqeWyZVSytqMdf9KcsJ6pVlDGnv71f968yHlNKeNC0JMmXN8gmUJ2YQibUPZkBVsyYLlFnEmpuRTdV5JhUwjMI7ndpfI9FCTbG8iYSThCH1fLh7v7L_OSDGGGtCd5nwtOpETCF_Lh7sfFJ3jZPPOwyfjq13vafH7_7vr8Q3u1vLg8P7tqgRtTWlRSGyOEB-hx5E5hvXrsnKADVRJNr5mXqJiUonfcS6lYxRw3tI7dK37aXB51xwhru01hqg3ZCMH-DMS0spBKcBu0atQMvNFIBy686AahvYLOa49Oy5FWrTdHrW2K33aYi13HXZpr-7bThishGWN_qBVU0TD7WBK4w1LtmVKCa9l3XaUW_6HqGXEKLs7oQ43_U0CPBS7FnBP638Mwag-e2-q55dIePLcHz_kjIEOefA</recordid><startdate>20231127</startdate><enddate>20231127</enddate><creator>Farmer, Nicholas</creator><creator>O'Neill, Hugh St. C</creator><general>Copernicus GmbH</general><general>Copernicus Publications</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>JG9</scope><scope>PCBAR</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0002-8658-4718</orcidid></search><sort><creationdate>20231127</creationdate><title>The miscibility gap between the rock salt and wurtzite phases in the MgO–ZnO binary system to 3.5 GPa</title><author>Farmer, Nicholas ; O'Neill, Hugh St. C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a399t-e7589944faa6ed3c7ec7e8d2c40b075e9681f5e715546c3f5571d3cc390202673</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Analysis</topic><topic>Binary system</topic><topic>Chemical properties</topic><topic>Composition</topic><topic>Equilibrium</topic><topic>Experiments</topic><topic>Gibbs free energy</topic><topic>Henrys law</topic><topic>Interstices</topic><topic>Magnesium compounds</topic><topic>Magnesium oxide</topic><topic>Miscibility</topic><topic>Molar volume</topic><topic>Phase transitions</topic><topic>Pressure</topic><topic>Raoults law</topic><topic>Rock-salt</topic><topic>Rocks</topic><topic>Salt</topic><topic>Salts</topic><topic>Solid solutions</topic><topic>Solubility</topic><topic>Temperature</topic><topic>Thermodynamic models</topic><topic>Thermodynamics</topic><topic>Wurtzite</topic><topic>X-ray diffraction</topic><topic>Zinc oxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Farmer, Nicholas</creatorcontrib><creatorcontrib>O'Neill, Hugh St. C</creatorcontrib><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest One Sustainability</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>ProQuest Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Research Database</collection><collection>ProQuest Earth, Atmospheric & Aquatic Science Database</collection><collection>Publicly Available Content (ProQuest)</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>Directory of Open Access Journals(OpenAccess)</collection><jtitle>European journal of mineralogy (Stuttgart)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Farmer, Nicholas</au><au>O'Neill, Hugh St. C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The miscibility gap between the rock salt and wurtzite phases in the MgO–ZnO binary system to 3.5 GPa</atitle><jtitle>European journal of mineralogy (Stuttgart)</jtitle><date>2023-11-27</date><risdate>2023</risdate><volume>35</volume><issue>6</issue><spage>1051</spage><epage>1071</epage><pages>1051-1071</pages><issn>1617-4011</issn><issn>0935-1221</issn><eissn>1617-4011</eissn><abstract>At ambient pressure, MgO crystallizes in the rock salt (B1) structure, whereas ZnO crystallizes in the wurtzite structure (B4). The asymmetric miscibility gap between these two structures in the MgO–ZnO binary system narrows with increasing pressure, terminating at the wurtzite-to-rock-salt phase transition in pure ZnO, which occurs at approximately 5 GPa at 1000 ∘C. Despite their essential simplicity, the pressure–temperature–composition (P–T–X) relations in the MgO–ZnO binary system have been sparsely studied experimentally, with disparate results that are inconsistent with available thermodynamic data. Here we report the experimental determination of the P–T–X relations of the miscibility gap from 940 to 1500 ∘C and 0 to 3.5 GPa, which we combine with calorimetric and equation-of-state data from the literature and on the transition in endmember ZnO, to build a thermodynamic model that resolves many of the inconsistencies. The model treats the rock salt phase as an ideal solution (no excess Gibbs free energy of mixing), while in the wurtzite phase the MgO component follows Henry's law and the ZnO component Raoult's law in the range of compositions accessed experimentally. However, there is an inconsistency between the partial molar volume of wurtzite-structured MgO deduced from this model and that inferred from lattice parameter measurements by X-ray diffraction in the quenched samples. This discrepancy may be caused by unquenchable disordering of some significant fraction of the substituting Mg2+ into normally vacant octahedral interstices of the wurtzite structure.</abstract><cop>Göttingen</cop><pub>Copernicus GmbH</pub><doi>10.5194/ejm-35-1051-2023</doi><tpages>21</tpages><orcidid>https://orcid.org/0000-0002-8658-4718</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Analysis Binary system Chemical properties Composition Equilibrium Experiments Gibbs free energy Henrys law Interstices Magnesium compounds Magnesium oxide Miscibility Molar volume Phase transitions Pressure Raoults law Rock-salt Rocks Salt Salts Solid solutions Solubility Temperature Thermodynamic models Thermodynamics Wurtzite X-ray diffraction Zinc oxide |
title | The miscibility gap between the rock salt and wurtzite phases in the MgO–ZnO binary system to 3.5 GPa |
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