Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O

► Refinement of phase diagram for the system Mg-Rh-O and thermodynamic data for spinel compounds MgRh 2O 4 and Mg 2RhO 4 is presented. ► A solid-state electrochemical cell is used for thermodynamic measurement. ► An advanced design of the solid-state electrochemical cell incorporating buffer electro...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Journal of alloys and compounds 2012-02, Vol.513, p.365-372
Hauptverfasser: Jacob, K.T., Prusty, Debadutta, Kale, G.M.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 372
container_issue
container_start_page 365
container_title Journal of alloys and compounds
container_volume 513
creator Jacob, K.T.
Prusty, Debadutta
Kale, G.M.
description ► Refinement of phase diagram for the system Mg-Rh-O and thermodynamic data for spinel compounds MgRh 2O 4 and Mg 2RhO 4 is presented. ► A solid-state electrochemical cell is used for thermodynamic measurement. ► An advanced design of the solid-state electrochemical cell incorporating buffer electrodes is deployed to minimize polarization of working electrode. ► Regular solution model for the spinel solid solution MgRh 2O 4 – Mg 2RhO 4 based on ideal mixing of cations on the octahedral site is proposed. ► Factors responsible for stabilization of tetravalent rhodium in spinel compounds are identified. Pure stoichiometric MgRh 2O 4 could not be prepared by solid state reaction from an equimolar mixture of MgO and Rh 2O 3 in air. The spinel phase formed always contained excess of Mg and traces of Rh or Rh 2O 3. The spinel phase can be considered as a solid solution of Mg 2RhO 4 in MgRh 2O 4. The compositions of the spinel solid solution in equilibrium with different phases in the ternary system Mg–Rh–O were determined by electron probe microanalysis. The oxygen potential established by the equilibrium between Rh + MgO + Mg 1+ x Rh 2− x O 4 was measured as a function of temperature using a solid-state cell incorporating yttria-stabilized zirconia as an electrolyte and pure oxygen at 0.1 MPa as the reference electrode. To avoid polarization of the working electrode during the measurements, an improved design of the cell with a buffer electrode was used. The standard Gibbs energies of formation of MgRh 2O 4 and Mg 2RhO 4 were deduced from the measured electromotive force (e.m.f.) by invoking a model for the spinel solid solution. The parameters of the model were optimized using the measured composition of the spinel solid solution in different phase fields and imposed oxygen partial pressures. The results can be summarized by the equations: MgO + β–Rh 2O 3 → MgRh 2O 4; ΔG ∘(± 1010)/J mol −1 = − 32239 + 7.534 T; 2MgO + RhO 2 → Mg 2RhO 4; ΔG ∘(± 1270)/J mol −1 = 36427 − 4.163 T; ΔG M /J mol −1 = 2RT( x In x + (1 − x)In(1 − x)) + 4650 x(1 − x), where Δ G° is the standard Gibbs free energy change for the reaction and Δ G M is the free energy of mixing of the spinel solid solution Mg 1+xRh 2− x O 4.
doi_str_mv 10.1016/j.jallcom.2011.10.050
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_1010881842</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S092583881102007X</els_id><sourcerecordid>1010881842</sourcerecordid><originalsourceid>FETCH-LOGICAL-c372t-629ddc4d897e94d226535e8a530d0a197d585738433ce1243d7d07436a87babd3</originalsourceid><addsrcrecordid>eNqFkMtKAzEUhoMoWC-PIGQjuJmay2QmsxIRb6BURNdDmpy2KelMzZkK7nwH39AnMeMUt27OgZ_vP5efkBPOxpzx4nw5XpoQbLsaC8Z50sZMsR0y4rqUWV4U1S4ZsUqoTEut98kB4pIxxivJR8Q8LQwCjRBM59sGqWkcvfXTKVJoIM49IG1nFNe-gUDXPTww2Ab_WzeDzze0WwDFD-xgRR_n359fz4tUJkdkb2YCwvG2H5LXm-uXq7vsYXJ7f3X5kFlZii4rROWczZ2uSqhyJ0ShpAJtlGSOGV6VTmlVSp1LaYGLXLrSsTKXhdHl1EydPCRnw9x1bN82gF298mghBNNAu8E6RcW05joXCVUDamOLGGFWr6NfmfiRoJ4r6mW9jbTuI-3lFGnynW5XGLQmzKJprMc_s1AqXVT03MXAQfr33UOs0XpoLDgfwXa1a_0_m34AYcqQVQ</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1010881842</pqid></control><display><type>article</type><title>Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O</title><source>Access via ScienceDirect (Elsevier)</source><creator>Jacob, K.T. ; Prusty, Debadutta ; Kale, G.M.</creator><creatorcontrib>Jacob, K.T. ; Prusty, Debadutta ; Kale, G.M.</creatorcontrib><description>► Refinement of phase diagram for the system Mg-Rh-O and thermodynamic data for spinel compounds MgRh 2O 4 and Mg 2RhO 4 is presented. ► A solid-state electrochemical cell is used for thermodynamic measurement. ► An advanced design of the solid-state electrochemical cell incorporating buffer electrodes is deployed to minimize polarization of working electrode. ► Regular solution model for the spinel solid solution MgRh 2O 4 – Mg 2RhO 4 based on ideal mixing of cations on the octahedral site is proposed. ► Factors responsible for stabilization of tetravalent rhodium in spinel compounds are identified. Pure stoichiometric MgRh 2O 4 could not be prepared by solid state reaction from an equimolar mixture of MgO and Rh 2O 3 in air. The spinel phase formed always contained excess of Mg and traces of Rh or Rh 2O 3. The spinel phase can be considered as a solid solution of Mg 2RhO 4 in MgRh 2O 4. The compositions of the spinel solid solution in equilibrium with different phases in the ternary system Mg–Rh–O were determined by electron probe microanalysis. The oxygen potential established by the equilibrium between Rh + MgO + Mg 1+ x Rh 2− x O 4 was measured as a function of temperature using a solid-state cell incorporating yttria-stabilized zirconia as an electrolyte and pure oxygen at 0.1 MPa as the reference electrode. To avoid polarization of the working electrode during the measurements, an improved design of the cell with a buffer electrode was used. The standard Gibbs energies of formation of MgRh 2O 4 and Mg 2RhO 4 were deduced from the measured electromotive force (e.m.f.) by invoking a model for the spinel solid solution. The parameters of the model were optimized using the measured composition of the spinel solid solution in different phase fields and imposed oxygen partial pressures. The results can be summarized by the equations: MgO + β–Rh 2O 3 → MgRh 2O 4; ΔG ∘(± 1010)/J mol −1 = − 32239 + 7.534 T; 2MgO + RhO 2 → Mg 2RhO 4; ΔG ∘(± 1270)/J mol −1 = 36427 − 4.163 T; ΔG M /J mol −1 = 2RT( x In x + (1 − x)In(1 − x)) + 4650 x(1 − x), where Δ G° is the standard Gibbs free energy change for the reaction and Δ G M is the free energy of mixing of the spinel solid solution Mg 1+xRh 2− x O 4.</description><identifier>ISSN: 0925-8388</identifier><identifier>EISSN: 1873-4669</identifier><identifier>DOI: 10.1016/j.jallcom.2011.10.050</identifier><language>eng</language><publisher>Kidlington: Elsevier B.V</publisher><subject>Condensed matter: structure, mechanical and thermal properties ; Cross-disciplinary physics: materials science; rheology ; Electrodes ; Electrolytic cells ; Electromotive force (e.m.f.) ; Enthalpy ; Entropy ; Exact sciences and technology ; Free energy ; Magnesium ; Magnesium oxide ; Magnesium rhodate (Mg 2RhO 4) ; Magnesium rhodite (MgRh 2O 4) ; Materials science ; Mathematical models ; Phase diagram ; Phase diagrams and microstructures developed by solidification and solid-solid phase transformations ; Phase diagrams of metals and alloys ; Physics ; Solid solution ; Solid solutions ; Spinel ; Spinels ; Stability ; Thermal properties of condensed matter ; Thermal properties of crystalline solids ; Thermodynamic properties ; Yttria stabilized zirconia</subject><ispartof>Journal of alloys and compounds, 2012-02, Vol.513, p.365-372</ispartof><rights>2011 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c372t-629ddc4d897e94d226535e8a530d0a197d585738433ce1243d7d07436a87babd3</citedby><cites>FETCH-LOGICAL-c372t-629ddc4d897e94d226535e8a530d0a197d585738433ce1243d7d07436a87babd3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jallcom.2011.10.050$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=25507460$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Jacob, K.T.</creatorcontrib><creatorcontrib>Prusty, Debadutta</creatorcontrib><creatorcontrib>Kale, G.M.</creatorcontrib><title>Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O</title><title>Journal of alloys and compounds</title><description>► Refinement of phase diagram for the system Mg-Rh-O and thermodynamic data for spinel compounds MgRh 2O 4 and Mg 2RhO 4 is presented. ► A solid-state electrochemical cell is used for thermodynamic measurement. ► An advanced design of the solid-state electrochemical cell incorporating buffer electrodes is deployed to minimize polarization of working electrode. ► Regular solution model for the spinel solid solution MgRh 2O 4 – Mg 2RhO 4 based on ideal mixing of cations on the octahedral site is proposed. ► Factors responsible for stabilization of tetravalent rhodium in spinel compounds are identified. Pure stoichiometric MgRh 2O 4 could not be prepared by solid state reaction from an equimolar mixture of MgO and Rh 2O 3 in air. The spinel phase formed always contained excess of Mg and traces of Rh or Rh 2O 3. The spinel phase can be considered as a solid solution of Mg 2RhO 4 in MgRh 2O 4. The compositions of the spinel solid solution in equilibrium with different phases in the ternary system Mg–Rh–O were determined by electron probe microanalysis. The oxygen potential established by the equilibrium between Rh + MgO + Mg 1+ x Rh 2− x O 4 was measured as a function of temperature using a solid-state cell incorporating yttria-stabilized zirconia as an electrolyte and pure oxygen at 0.1 MPa as the reference electrode. To avoid polarization of the working electrode during the measurements, an improved design of the cell with a buffer electrode was used. The standard Gibbs energies of formation of MgRh 2O 4 and Mg 2RhO 4 were deduced from the measured electromotive force (e.m.f.) by invoking a model for the spinel solid solution. The parameters of the model were optimized using the measured composition of the spinel solid solution in different phase fields and imposed oxygen partial pressures. The results can be summarized by the equations: MgO + β–Rh 2O 3 → MgRh 2O 4; ΔG ∘(± 1010)/J mol −1 = − 32239 + 7.534 T; 2MgO + RhO 2 → Mg 2RhO 4; ΔG ∘(± 1270)/J mol −1 = 36427 − 4.163 T; ΔG M /J mol −1 = 2RT( x In x + (1 − x)In(1 − x)) + 4650 x(1 − x), where Δ G° is the standard Gibbs free energy change for the reaction and Δ G M is the free energy of mixing of the spinel solid solution Mg 1+xRh 2− x O 4.</description><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Electrodes</subject><subject>Electrolytic cells</subject><subject>Electromotive force (e.m.f.)</subject><subject>Enthalpy</subject><subject>Entropy</subject><subject>Exact sciences and technology</subject><subject>Free energy</subject><subject>Magnesium</subject><subject>Magnesium oxide</subject><subject>Magnesium rhodate (Mg 2RhO 4)</subject><subject>Magnesium rhodite (MgRh 2O 4)</subject><subject>Materials science</subject><subject>Mathematical models</subject><subject>Phase diagram</subject><subject>Phase diagrams and microstructures developed by solidification and solid-solid phase transformations</subject><subject>Phase diagrams of metals and alloys</subject><subject>Physics</subject><subject>Solid solution</subject><subject>Solid solutions</subject><subject>Spinel</subject><subject>Spinels</subject><subject>Stability</subject><subject>Thermal properties of condensed matter</subject><subject>Thermal properties of crystalline solids</subject><subject>Thermodynamic properties</subject><subject>Yttria stabilized zirconia</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNqFkMtKAzEUhoMoWC-PIGQjuJmay2QmsxIRb6BURNdDmpy2KelMzZkK7nwH39AnMeMUt27OgZ_vP5efkBPOxpzx4nw5XpoQbLsaC8Z50sZMsR0y4rqUWV4U1S4ZsUqoTEut98kB4pIxxivJR8Q8LQwCjRBM59sGqWkcvfXTKVJoIM49IG1nFNe-gUDXPTww2Ab_WzeDzze0WwDFD-xgRR_n359fz4tUJkdkb2YCwvG2H5LXm-uXq7vsYXJ7f3X5kFlZii4rROWczZ2uSqhyJ0ShpAJtlGSOGV6VTmlVSp1LaYGLXLrSsTKXhdHl1EydPCRnw9x1bN82gF298mghBNNAu8E6RcW05joXCVUDamOLGGFWr6NfmfiRoJ4r6mW9jbTuI-3lFGnynW5XGLQmzKJprMc_s1AqXVT03MXAQfr33UOs0XpoLDgfwXa1a_0_m34AYcqQVQ</recordid><startdate>20120205</startdate><enddate>20120205</enddate><creator>Jacob, K.T.</creator><creator>Prusty, Debadutta</creator><creator>Kale, G.M.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20120205</creationdate><title>Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O</title><author>Jacob, K.T. ; Prusty, Debadutta ; Kale, G.M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c372t-629ddc4d897e94d226535e8a530d0a197d585738433ce1243d7d07436a87babd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Electrodes</topic><topic>Electrolytic cells</topic><topic>Electromotive force (e.m.f.)</topic><topic>Enthalpy</topic><topic>Entropy</topic><topic>Exact sciences and technology</topic><topic>Free energy</topic><topic>Magnesium</topic><topic>Magnesium oxide</topic><topic>Magnesium rhodate (Mg 2RhO 4)</topic><topic>Magnesium rhodite (MgRh 2O 4)</topic><topic>Materials science</topic><topic>Mathematical models</topic><topic>Phase diagram</topic><topic>Phase diagrams and microstructures developed by solidification and solid-solid phase transformations</topic><topic>Phase diagrams of metals and alloys</topic><topic>Physics</topic><topic>Solid solution</topic><topic>Solid solutions</topic><topic>Spinel</topic><topic>Spinels</topic><topic>Stability</topic><topic>Thermal properties of condensed matter</topic><topic>Thermal properties of crystalline solids</topic><topic>Thermodynamic properties</topic><topic>Yttria stabilized zirconia</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Jacob, K.T.</creatorcontrib><creatorcontrib>Prusty, Debadutta</creatorcontrib><creatorcontrib>Kale, G.M.</creatorcontrib><collection>Pascal-Francis</collection><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>Jacob, K.T.</au><au>Prusty, Debadutta</au><au>Kale, G.M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2012-02-05</date><risdate>2012</risdate><volume>513</volume><spage>365</spage><epage>372</epage><pages>365-372</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>► Refinement of phase diagram for the system Mg-Rh-O and thermodynamic data for spinel compounds MgRh 2O 4 and Mg 2RhO 4 is presented. ► A solid-state electrochemical cell is used for thermodynamic measurement. ► An advanced design of the solid-state electrochemical cell incorporating buffer electrodes is deployed to minimize polarization of working electrode. ► Regular solution model for the spinel solid solution MgRh 2O 4 – Mg 2RhO 4 based on ideal mixing of cations on the octahedral site is proposed. ► Factors responsible for stabilization of tetravalent rhodium in spinel compounds are identified. Pure stoichiometric MgRh 2O 4 could not be prepared by solid state reaction from an equimolar mixture of MgO and Rh 2O 3 in air. The spinel phase formed always contained excess of Mg and traces of Rh or Rh 2O 3. The spinel phase can be considered as a solid solution of Mg 2RhO 4 in MgRh 2O 4. The compositions of the spinel solid solution in equilibrium with different phases in the ternary system Mg–Rh–O were determined by electron probe microanalysis. The oxygen potential established by the equilibrium between Rh + MgO + Mg 1+ x Rh 2− x O 4 was measured as a function of temperature using a solid-state cell incorporating yttria-stabilized zirconia as an electrolyte and pure oxygen at 0.1 MPa as the reference electrode. To avoid polarization of the working electrode during the measurements, an improved design of the cell with a buffer electrode was used. The standard Gibbs energies of formation of MgRh 2O 4 and Mg 2RhO 4 were deduced from the measured electromotive force (e.m.f.) by invoking a model for the spinel solid solution. The parameters of the model were optimized using the measured composition of the spinel solid solution in different phase fields and imposed oxygen partial pressures. The results can be summarized by the equations: MgO + β–Rh 2O 3 → MgRh 2O 4; ΔG ∘(± 1010)/J mol −1 = − 32239 + 7.534 T; 2MgO + RhO 2 → Mg 2RhO 4; ΔG ∘(± 1270)/J mol −1 = 36427 − 4.163 T; ΔG M /J mol −1 = 2RT( x In x + (1 − x)In(1 − x)) + 4650 x(1 − x), where Δ G° is the standard Gibbs free energy change for the reaction and Δ G M is the free energy of mixing of the spinel solid solution Mg 1+xRh 2− x O 4.</abstract><cop>Kidlington</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jallcom.2011.10.050</doi><tpages>8</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0925-8388
ispartof Journal of alloys and compounds, 2012-02, Vol.513, p.365-372
issn 0925-8388
1873-4669
language eng
recordid cdi_proquest_miscellaneous_1010881842
source Access via ScienceDirect (Elsevier)
subjects Condensed matter: structure, mechanical and thermal properties
Cross-disciplinary physics: materials science
rheology
Electrodes
Electrolytic cells
Electromotive force (e.m.f.)
Enthalpy
Entropy
Exact sciences and technology
Free energy
Magnesium
Magnesium oxide
Magnesium rhodate (Mg 2RhO 4)
Magnesium rhodite (MgRh 2O 4)
Materials science
Mathematical models
Phase diagram
Phase diagrams and microstructures developed by solidification and solid-solid phase transformations
Phase diagrams of metals and alloys
Physics
Solid solution
Solid solutions
Spinel
Spinels
Stability
Thermal properties of condensed matter
Thermal properties of crystalline solids
Thermodynamic properties
Yttria stabilized zirconia
title Phase relations and Gibbs energies of spinel phases and solid solutions in the system Mg–Rh–O
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-23T12%3A24%3A04IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Phase%20relations%20and%20Gibbs%20energies%20of%20spinel%20phases%20and%20solid%20solutions%20in%20the%20system%20Mg%E2%80%93Rh%E2%80%93O&rft.jtitle=Journal%20of%20alloys%20and%20compounds&rft.au=Jacob,%20K.T.&rft.date=2012-02-05&rft.volume=513&rft.spage=365&rft.epage=372&rft.pages=365-372&rft.issn=0925-8388&rft.eissn=1873-4669&rft_id=info:doi/10.1016/j.jallcom.2011.10.050&rft_dat=%3Cproquest_cross%3E1010881842%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=1010881842&rft_id=info:pmid/&rft_els_id=S092583881102007X&rfr_iscdi=true