Phase Equilibria in the Cu2S-Cu8SiS6-Cu8GeS6 System and Thermodynamic Functions of Phase Transitions of the Cu8Si(1−X)GeXS6 Argyrodite Phases
The phase equilibria of the Cu 2 S-SiS 2 -GeS 2 system have been studied in the Cu 2 S-Cu 8 SiS 6 -Cu 8 GeS 6 composition area. Based on data obtained from differential thermal analysis, powder x-ray diffraction, and SEM-EDS techniques, the T-x diagram of the Cu 8 SiS 6 -Cu 8 GeS 6 boundary system a...
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creator | Bayramova, Ulviyya R. Babanly, Kamala N. Ahmadov, Eldar I. Mashadiyeva, Leyla F. Babanly, Mahammad B. |
description | The phase equilibria of the Cu
2
S-SiS
2
-GeS
2
system have been studied in the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
composition area. Based on data obtained from differential thermal analysis, powder x-ray diffraction, and SEM-EDS techniques, the T-x diagram of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system and two internal polythermal sections, as well as the isothermal section at 300 K of the phase diagram and the liquidus surface of the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
system were constructed. The areas of primary crystallization and homogeneity of phases, the nature, and temperatures of invariant and monovariant equilibria were determined. Continuous solid solutions based on both crystalline modifications of the starting compounds of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system, have been revealed, which are of interest as environmentally friendly functional materials. The temperatures and enthalpies of phase transitions of Cu
8
SiS
6
and Cu
8
GeS
6
compounds, and Cu
8
Si
(1−
X
)
Ge
X
S
6
solid solutions were determined using differential scanning calorimetry. The entropies of phase transitions for end-member compounds were also calculated. It is shown that the heats and entropies of phase transitions of these phases are anomalously large in comparison with the thermodynamic functions of ordinary polymorphic transitions. Apparently, this is due to a significant increase in the degree of disorder in the cationic sublattice upon transition to the high-temperature ion-conducting phase. It has also been established that the heats of phase transitions of solid solutions are practically equal to the sum of the corresponding functions of the end-member compounds. |
doi_str_mv | 10.1007/s11669-023-01054-y |
format | Article |
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2
S-SiS
2
-GeS
2
system have been studied in the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
composition area. Based on data obtained from differential thermal analysis, powder x-ray diffraction, and SEM-EDS techniques, the T-x diagram of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system and two internal polythermal sections, as well as the isothermal section at 300 K of the phase diagram and the liquidus surface of the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
system were constructed. The areas of primary crystallization and homogeneity of phases, the nature, and temperatures of invariant and monovariant equilibria were determined. Continuous solid solutions based on both crystalline modifications of the starting compounds of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system, have been revealed, which are of interest as environmentally friendly functional materials. The temperatures and enthalpies of phase transitions of Cu
8
SiS
6
and Cu
8
GeS
6
compounds, and Cu
8
Si
(1−
X
)
Ge
X
S
6
solid solutions were determined using differential scanning calorimetry. The entropies of phase transitions for end-member compounds were also calculated. It is shown that the heats and entropies of phase transitions of these phases are anomalously large in comparison with the thermodynamic functions of ordinary polymorphic transitions. Apparently, this is due to a significant increase in the degree of disorder in the cationic sublattice upon transition to the high-temperature ion-conducting phase. It has also been established that the heats of phase transitions of solid solutions are practically equal to the sum of the corresponding functions of the end-member compounds.</description><identifier>ISSN: 1547-7037</identifier><identifier>EISSN: 1863-7345</identifier><identifier>EISSN: 1934-7243</identifier><identifier>DOI: 10.1007/s11669-023-01054-y</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Ceramics ; Composites ; Copper sulfides ; Crystallization ; Crystallography and Scattering Methods ; Differential thermal analysis ; Engineering Thermodynamics ; Enthalpy ; Equilibrium ; Functional materials ; Glass ; Heat and Mass Transfer ; Heat transmission ; High temperature ; Homogeneity ; Liquidus ; Mathematical analysis ; Metallic Materials ; Natural Materials ; Original Research Article ; Phase diagrams ; Phase equilibria ; Phase transitions ; Phases ; Physics ; Physics and Astronomy ; Solid solutions ; Thermodynamics ; X ray powder diffraction</subject><ispartof>Journal of phase equilibria and diffusion, 2023-06, Vol.44 (3), p.509-519</ispartof><rights>ASM International 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c319t-b8a3f60e80bb4c00992dbee57bd957c5a98e16aad882694b756d30fdeeaf2f23</citedby><cites>FETCH-LOGICAL-c319t-b8a3f60e80bb4c00992dbee57bd957c5a98e16aad882694b756d30fdeeaf2f23</cites><orcidid>0000-0001-5962-3710</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11669-023-01054-y$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11669-023-01054-y$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,41467,42536,51297</link.rule.ids></links><search><creatorcontrib>Bayramova, Ulviyya R.</creatorcontrib><creatorcontrib>Babanly, Kamala N.</creatorcontrib><creatorcontrib>Ahmadov, Eldar I.</creatorcontrib><creatorcontrib>Mashadiyeva, Leyla F.</creatorcontrib><creatorcontrib>Babanly, Mahammad B.</creatorcontrib><title>Phase Equilibria in the Cu2S-Cu8SiS6-Cu8GeS6 System and Thermodynamic Functions of Phase Transitions of the Cu8Si(1−X)GeXS6 Argyrodite Phases</title><title>Journal of phase equilibria and diffusion</title><addtitle>J. Phase Equilib. Diffus</addtitle><description>The phase equilibria of the Cu
2
S-SiS
2
-GeS
2
system have been studied in the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
composition area. Based on data obtained from differential thermal analysis, powder x-ray diffraction, and SEM-EDS techniques, the T-x diagram of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system and two internal polythermal sections, as well as the isothermal section at 300 K of the phase diagram and the liquidus surface of the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
system were constructed. The areas of primary crystallization and homogeneity of phases, the nature, and temperatures of invariant and monovariant equilibria were determined. Continuous solid solutions based on both crystalline modifications of the starting compounds of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system, have been revealed, which are of interest as environmentally friendly functional materials. The temperatures and enthalpies of phase transitions of Cu
8
SiS
6
and Cu
8
GeS
6
compounds, and Cu
8
Si
(1−
X
)
Ge
X
S
6
solid solutions were determined using differential scanning calorimetry. The entropies of phase transitions for end-member compounds were also calculated. It is shown that the heats and entropies of phase transitions of these phases are anomalously large in comparison with the thermodynamic functions of ordinary polymorphic transitions. Apparently, this is due to a significant increase in the degree of disorder in the cationic sublattice upon transition to the high-temperature ion-conducting phase. It has also been established that the heats of phase transitions of solid solutions are practically equal to the sum of the corresponding functions of the end-member compounds.</description><subject>Ceramics</subject><subject>Composites</subject><subject>Copper sulfides</subject><subject>Crystallization</subject><subject>Crystallography and Scattering Methods</subject><subject>Differential thermal analysis</subject><subject>Engineering Thermodynamics</subject><subject>Enthalpy</subject><subject>Equilibrium</subject><subject>Functional materials</subject><subject>Glass</subject><subject>Heat and Mass Transfer</subject><subject>Heat transmission</subject><subject>High temperature</subject><subject>Homogeneity</subject><subject>Liquidus</subject><subject>Mathematical analysis</subject><subject>Metallic Materials</subject><subject>Natural Materials</subject><subject>Original Research Article</subject><subject>Phase diagrams</subject><subject>Phase equilibria</subject><subject>Phase transitions</subject><subject>Phases</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Solid solutions</subject><subject>Thermodynamics</subject><subject>X ray powder diffraction</subject><issn>1547-7037</issn><issn>1863-7345</issn><issn>1934-7243</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kMtKw0AUhoMoWKsv4GrAjS5G55LMZSnFVqGgkCy6GybJSTtikzqTLPIG7gQf0ScxNaI7V-dw-L_vwB9F55RcU0LkTaBUCI0J45hQksS4P4gmVAmOJY-Tw2FPYokl4fI4OgnhmRCmpRKT6P1pYwOgu9fOvbjcO4tcjdoNoFnHUjzrVOpSsZ8LSAVK-9DCFtm6RNkG_LYp-9puXYHmXV20rqkDaio0KjNv6-B-j6Nz0F3Sz7eP1dUCVoPw1q9735SuhZEKp9FRZV8CnP3MaZTN77LZPV4-Lh5mt0tccKpbnCvLK0FAkTyPC0K0ZmUOkMi81IksEqsVUGFtqRQTOs5lIkpOqhLAVqxifBpdjNqdb147CK15bjpfDx8NU4IlSpOYDyk2pgrfhOChMjvvttb3hhKz792MvZuhd_Pdu-kHiI9QGML1Gvyf-h_qC7X9h3M</recordid><startdate>20230601</startdate><enddate>20230601</enddate><creator>Bayramova, Ulviyya R.</creator><creator>Babanly, Kamala N.</creator><creator>Ahmadov, Eldar I.</creator><creator>Mashadiyeva, Leyla F.</creator><creator>Babanly, Mahammad B.</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>U9A</scope><orcidid>https://orcid.org/0000-0001-5962-3710</orcidid></search><sort><creationdate>20230601</creationdate><title>Phase Equilibria in the Cu2S-Cu8SiS6-Cu8GeS6 System and Thermodynamic Functions of Phase Transitions of the Cu8Si(1−X)GeXS6 Argyrodite Phases</title><author>Bayramova, Ulviyya R. ; Babanly, Kamala N. ; Ahmadov, Eldar I. ; Mashadiyeva, Leyla F. ; Babanly, Mahammad B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c319t-b8a3f60e80bb4c00992dbee57bd957c5a98e16aad882694b756d30fdeeaf2f23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Ceramics</topic><topic>Composites</topic><topic>Copper sulfides</topic><topic>Crystallization</topic><topic>Crystallography and Scattering Methods</topic><topic>Differential thermal analysis</topic><topic>Engineering Thermodynamics</topic><topic>Enthalpy</topic><topic>Equilibrium</topic><topic>Functional materials</topic><topic>Glass</topic><topic>Heat and Mass Transfer</topic><topic>Heat transmission</topic><topic>High temperature</topic><topic>Homogeneity</topic><topic>Liquidus</topic><topic>Mathematical analysis</topic><topic>Metallic Materials</topic><topic>Natural Materials</topic><topic>Original Research Article</topic><topic>Phase diagrams</topic><topic>Phase equilibria</topic><topic>Phase transitions</topic><topic>Phases</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Solid solutions</topic><topic>Thermodynamics</topic><topic>X ray powder diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bayramova, Ulviyya R.</creatorcontrib><creatorcontrib>Babanly, Kamala N.</creatorcontrib><creatorcontrib>Ahmadov, Eldar I.</creatorcontrib><creatorcontrib>Mashadiyeva, Leyla F.</creatorcontrib><creatorcontrib>Babanly, Mahammad B.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of phase equilibria and diffusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bayramova, Ulviyya R.</au><au>Babanly, Kamala N.</au><au>Ahmadov, Eldar I.</au><au>Mashadiyeva, Leyla F.</au><au>Babanly, Mahammad B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Phase Equilibria in the Cu2S-Cu8SiS6-Cu8GeS6 System and Thermodynamic Functions of Phase Transitions of the Cu8Si(1−X)GeXS6 Argyrodite Phases</atitle><jtitle>Journal of phase equilibria and diffusion</jtitle><stitle>J. Phase Equilib. Diffus</stitle><date>2023-06-01</date><risdate>2023</risdate><volume>44</volume><issue>3</issue><spage>509</spage><epage>519</epage><pages>509-519</pages><issn>1547-7037</issn><eissn>1863-7345</eissn><eissn>1934-7243</eissn><abstract>The phase equilibria of the Cu
2
S-SiS
2
-GeS
2
system have been studied in the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
composition area. Based on data obtained from differential thermal analysis, powder x-ray diffraction, and SEM-EDS techniques, the T-x diagram of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system and two internal polythermal sections, as well as the isothermal section at 300 K of the phase diagram and the liquidus surface of the Cu
2
S-Cu
8
SiS
6
-Cu
8
GeS
6
system were constructed. The areas of primary crystallization and homogeneity of phases, the nature, and temperatures of invariant and monovariant equilibria were determined. Continuous solid solutions based on both crystalline modifications of the starting compounds of the Cu
8
SiS
6
-Cu
8
GeS
6
boundary system, have been revealed, which are of interest as environmentally friendly functional materials. The temperatures and enthalpies of phase transitions of Cu
8
SiS
6
and Cu
8
GeS
6
compounds, and Cu
8
Si
(1−
X
)
Ge
X
S
6
solid solutions were determined using differential scanning calorimetry. The entropies of phase transitions for end-member compounds were also calculated. It is shown that the heats and entropies of phase transitions of these phases are anomalously large in comparison with the thermodynamic functions of ordinary polymorphic transitions. Apparently, this is due to a significant increase in the degree of disorder in the cationic sublattice upon transition to the high-temperature ion-conducting phase. It has also been established that the heats of phase transitions of solid solutions are practically equal to the sum of the corresponding functions of the end-member compounds.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11669-023-01054-y</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0001-5962-3710</orcidid></addata></record> |
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issn | 1547-7037 1863-7345 1934-7243 |
language | eng |
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source | SpringerLink Journals - AutoHoldings |
subjects | Ceramics Composites Copper sulfides Crystallization Crystallography and Scattering Methods Differential thermal analysis Engineering Thermodynamics Enthalpy Equilibrium Functional materials Glass Heat and Mass Transfer Heat transmission High temperature Homogeneity Liquidus Mathematical analysis Metallic Materials Natural Materials Original Research Article Phase diagrams Phase equilibria Phase transitions Phases Physics Physics and Astronomy Solid solutions Thermodynamics X ray powder diffraction |
title | Phase Equilibria in the Cu2S-Cu8SiS6-Cu8GeS6 System and Thermodynamic Functions of Phase Transitions of the Cu8Si(1−X)GeXS6 Argyrodite Phases |
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