Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition
The variations of the bulk composition of the silicate Moon (crust + mantle = Bulk Silicate Moon, BSM) depending on the thermal state are explored based on the joint inversion of gravitational, seismic, and petrologic data within the Na 2 O–TiO 2 –CaO–FeO–MgO–Al 2 O 3 –SiO 2 system. The mantle bulk...
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description | The variations of the bulk composition of the silicate Moon (crust + mantle = Bulk Silicate Moon, BSM) depending on the thermal state are explored based on the joint inversion of gravitational, seismic, and petrologic data within the Na
2
O–TiO
2
–CaO–FeO–MgO–Al
2
O
3
–SiO
2
system. The mantle bulk temperature
T
mean
determining the mineral composition and physical properties of the Moon is adopted as the integral characteristic of thermal state. By parameter
T
mean
, all thermal models of the Moon can be conventionally broken down into the “cold” with
T
mean
~ 690–860°C and the “hot” with
T
mean
~ 925–1075°C. The estimations of refractory oxide abundance in lunar rocks depending on the thermal state are included in two different groups. Cold models of BSM are comparable by the bulk content of Al
2
O
3
~ 3.0–4.6 wt % to those for the silicate Earth (Bulk Silicate Earth, BSE), while hot models of BSM are significantly enriched with Al
2
O
3
~ 5.1–7.3 wt % (Al
2
O
3
~ 1.2–1.7 × BSE) as compared with BSE. On the contrary, independent of the temperature distribution, both types of BSM models are characterized by nearly constant values of bulk concentrations of FeO ~ 12–13 wt % and magnesian number MG# 80–81.5 (MG# = [MgO/(MgO + FeO) × 100]), which differ markedly from those for BSE (FeO ~ 8% and MG# 89). It means that for all possible temperature distributions, the silicate fraction of the Moon is FeO-enriched and MgO-depleted in relation to BSE. These arguments discard the possibility of the Moon’s formation out of the material of the Earth’s primitive mantle. In spite of the almost complete coincidence of the isotopic systems, this apparently undeniable fact has no adequate explanation in the existing canonical models of the Moon’s origin and should result in additional constraints on the dynamic processes in models of the formation of the Earth–Moon system. However, the problem of the similarity of and/or difference between compositions of the Moon and the Earth regarding the abundance of refractory elements, which is very important for the geochemistry of the Moon and the Earth’s mantle, remains unresolved and requires further study. |
doi_str_mv | 10.1134/S0038094618060047 |
format | Article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_journals_2138603352</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2138603352</sourcerecordid><originalsourceid>FETCH-LOGICAL-c316t-da463b69c5883e82d00e9279fe13efc60fab34230577163ca3ca5a2fbc794f1a3</originalsourceid><addsrcrecordid>eNp1kLFOwzAQhi0EEqXwAGyWmAPnOHEcNqigrdSKAZgjx7FpSmoX2x3Y-g5MvF6fBIciMSCkk0667__vdD9C5wQuCaHZ1SMA5VBmjHBgAFlxgAaEAU9oltJDNOhx0vNjdOL9EoAAFGyAxFhZuVCrVooOj6zxwYnWBI-twWGh4qhrsDANntiA57ZRXUT6G82tNbvtp8dTE5RrrbvGZLf9uN10r9G2WlvfhtaaU3SkRefV2U8fouf7u6fRJJk9jKejm1kiKWEhaUTGaM1KmXNOFU8bAFWmRakVoUpLBlrU_S-QFwVhVIpYuUh1LYsy00TQIbrY7107-7ZRPlRLu3EmnqxSQjkDSvM0qsheJZ313ildrV27Eu69IlD1SVZ_koyedO_xUWtelPvd_L_pC03jdgo</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2138603352</pqid></control><display><type>article</type><title>Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition</title><source>Springer Nature</source><creator>Kuskov, O. L. ; Kronrod, E. V. ; Kronrod, V. A.</creator><creatorcontrib>Kuskov, O. L. ; Kronrod, E. V. ; Kronrod, V. A.</creatorcontrib><description>The variations of the bulk composition of the silicate Moon (crust + mantle = Bulk Silicate Moon, BSM) depending on the thermal state are explored based on the joint inversion of gravitational, seismic, and petrologic data within the Na
2
O–TiO
2
–CaO–FeO–MgO–Al
2
O
3
–SiO
2
system. The mantle bulk temperature
T
mean
determining the mineral composition and physical properties of the Moon is adopted as the integral characteristic of thermal state. By parameter
T
mean
, all thermal models of the Moon can be conventionally broken down into the “cold” with
T
mean
~ 690–860°C and the “hot” with
T
mean
~ 925–1075°C. The estimations of refractory oxide abundance in lunar rocks depending on the thermal state are included in two different groups. Cold models of BSM are comparable by the bulk content of Al
2
O
3
~ 3.0–4.6 wt % to those for the silicate Earth (Bulk Silicate Earth, BSE), while hot models of BSM are significantly enriched with Al
2
O
3
~ 5.1–7.3 wt % (Al
2
O
3
~ 1.2–1.7 × BSE) as compared with BSE. On the contrary, independent of the temperature distribution, both types of BSM models are characterized by nearly constant values of bulk concentrations of FeO ~ 12–13 wt % and magnesian number MG# 80–81.5 (MG# = [MgO/(MgO + FeO) × 100]), which differ markedly from those for BSE (FeO ~ 8% and MG# 89). It means that for all possible temperature distributions, the silicate fraction of the Moon is FeO-enriched and MgO-depleted in relation to BSE. These arguments discard the possibility of the Moon’s formation out of the material of the Earth’s primitive mantle. In spite of the almost complete coincidence of the isotopic systems, this apparently undeniable fact has no adequate explanation in the existing canonical models of the Moon’s origin and should result in additional constraints on the dynamic processes in models of the formation of the Earth–Moon system. However, the problem of the similarity of and/or difference between compositions of the Moon and the Earth regarding the abundance of refractory elements, which is very important for the geochemistry of the Moon and the Earth’s mantle, remains unresolved and requires further study.</description><identifier>ISSN: 0038-0946</identifier><identifier>EISSN: 1608-3423</identifier><identifier>DOI: 10.1134/S0038094618060047</identifier><language>eng</language><publisher>Moscow: Pleiades Publishing</publisher><subject>Abundance ; Aluminum oxide ; Astronomy ; Astrophysics and Astroparticles ; Astrophysics and Cosmology ; Cold ; Composition ; Constraint modelling ; Crystallization ; Earth ; Earth mantle ; Geochemistry ; Lunar rocks ; Magnesium oxide ; Mineral composition ; Moon ; Observations and Techniques ; Physical properties ; Physics ; Physics and Astronomy ; Planetology ; Seismic surveys ; Silicon dioxide ; Solar system ; Temperature distribution ; Thermal analysis ; Thermal models ; Titanium dioxide</subject><ispartof>Solar system research, 2018-11, Vol.52 (6), p.467-479</ispartof><rights>Pleiades Publishing, Inc. 2018</rights><rights>Solar System Research is a copyright of Springer, (2018). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c316t-da463b69c5883e82d00e9279fe13efc60fab34230577163ca3ca5a2fbc794f1a3</citedby><cites>FETCH-LOGICAL-c316t-da463b69c5883e82d00e9279fe13efc60fab34230577163ca3ca5a2fbc794f1a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1134/S0038094618060047$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1134/S0038094618060047$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Kuskov, O. L.</creatorcontrib><creatorcontrib>Kronrod, E. V.</creatorcontrib><creatorcontrib>Kronrod, V. A.</creatorcontrib><title>Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition</title><title>Solar system research</title><addtitle>Sol Syst Res</addtitle><description>The variations of the bulk composition of the silicate Moon (crust + mantle = Bulk Silicate Moon, BSM) depending on the thermal state are explored based on the joint inversion of gravitational, seismic, and petrologic data within the Na
2
O–TiO
2
–CaO–FeO–MgO–Al
2
O
3
–SiO
2
system. The mantle bulk temperature
T
mean
determining the mineral composition and physical properties of the Moon is adopted as the integral characteristic of thermal state. By parameter
T
mean
, all thermal models of the Moon can be conventionally broken down into the “cold” with
T
mean
~ 690–860°C and the “hot” with
T
mean
~ 925–1075°C. The estimations of refractory oxide abundance in lunar rocks depending on the thermal state are included in two different groups. Cold models of BSM are comparable by the bulk content of Al
2
O
3
~ 3.0–4.6 wt % to those for the silicate Earth (Bulk Silicate Earth, BSE), while hot models of BSM are significantly enriched with Al
2
O
3
~ 5.1–7.3 wt % (Al
2
O
3
~ 1.2–1.7 × BSE) as compared with BSE. On the contrary, independent of the temperature distribution, both types of BSM models are characterized by nearly constant values of bulk concentrations of FeO ~ 12–13 wt % and magnesian number MG# 80–81.5 (MG# = [MgO/(MgO + FeO) × 100]), which differ markedly from those for BSE (FeO ~ 8% and MG# 89). It means that for all possible temperature distributions, the silicate fraction of the Moon is FeO-enriched and MgO-depleted in relation to BSE. These arguments discard the possibility of the Moon’s formation out of the material of the Earth’s primitive mantle. In spite of the almost complete coincidence of the isotopic systems, this apparently undeniable fact has no adequate explanation in the existing canonical models of the Moon’s origin and should result in additional constraints on the dynamic processes in models of the formation of the Earth–Moon system. However, the problem of the similarity of and/or difference between compositions of the Moon and the Earth regarding the abundance of refractory elements, which is very important for the geochemistry of the Moon and the Earth’s mantle, remains unresolved and requires further study.</description><subject>Abundance</subject><subject>Aluminum oxide</subject><subject>Astronomy</subject><subject>Astrophysics and Astroparticles</subject><subject>Astrophysics and Cosmology</subject><subject>Cold</subject><subject>Composition</subject><subject>Constraint modelling</subject><subject>Crystallization</subject><subject>Earth</subject><subject>Earth mantle</subject><subject>Geochemistry</subject><subject>Lunar rocks</subject><subject>Magnesium oxide</subject><subject>Mineral composition</subject><subject>Moon</subject><subject>Observations and Techniques</subject><subject>Physical properties</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Planetology</subject><subject>Seismic surveys</subject><subject>Silicon dioxide</subject><subject>Solar system</subject><subject>Temperature distribution</subject><subject>Thermal analysis</subject><subject>Thermal models</subject><subject>Titanium dioxide</subject><issn>0038-0946</issn><issn>1608-3423</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><recordid>eNp1kLFOwzAQhi0EEqXwAGyWmAPnOHEcNqigrdSKAZgjx7FpSmoX2x3Y-g5MvF6fBIciMSCkk0667__vdD9C5wQuCaHZ1SMA5VBmjHBgAFlxgAaEAU9oltJDNOhx0vNjdOL9EoAAFGyAxFhZuVCrVooOj6zxwYnWBI-twWGh4qhrsDANntiA57ZRXUT6G82tNbvtp8dTE5RrrbvGZLf9uN10r9G2WlvfhtaaU3SkRefV2U8fouf7u6fRJJk9jKejm1kiKWEhaUTGaM1KmXNOFU8bAFWmRakVoUpLBlrU_S-QFwVhVIpYuUh1LYsy00TQIbrY7107-7ZRPlRLu3EmnqxSQjkDSvM0qsheJZ313ildrV27Eu69IlD1SVZ_koyedO_xUWtelPvd_L_pC03jdgo</recordid><startdate>20181101</startdate><enddate>20181101</enddate><creator>Kuskov, O. L.</creator><creator>Kronrod, E. V.</creator><creator>Kronrod, V. A.</creator><general>Pleiades Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TG</scope><scope>7XB</scope><scope>88I</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>GNUQQ</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L7M</scope><scope>M2P</scope><scope>P5Z</scope><scope>P62</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>Q9U</scope></search><sort><creationdate>20181101</creationdate><title>Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition</title><author>Kuskov, O. L. ; Kronrod, E. V. ; Kronrod, V. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c316t-da463b69c5883e82d00e9279fe13efc60fab34230577163ca3ca5a2fbc794f1a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Abundance</topic><topic>Aluminum oxide</topic><topic>Astronomy</topic><topic>Astrophysics and Astroparticles</topic><topic>Astrophysics and Cosmology</topic><topic>Cold</topic><topic>Composition</topic><topic>Constraint modelling</topic><topic>Crystallization</topic><topic>Earth</topic><topic>Earth mantle</topic><topic>Geochemistry</topic><topic>Lunar rocks</topic><topic>Magnesium oxide</topic><topic>Mineral composition</topic><topic>Moon</topic><topic>Observations and Techniques</topic><topic>Physical properties</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Planetology</topic><topic>Seismic surveys</topic><topic>Silicon dioxide</topic><topic>Solar system</topic><topic>Temperature distribution</topic><topic>Thermal analysis</topic><topic>Thermal models</topic><topic>Titanium dioxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kuskov, O. L.</creatorcontrib><creatorcontrib>Kronrod, E. V.</creatorcontrib><creatorcontrib>Kronrod, V. A.</creatorcontrib><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>ProQuest Central Student</collection><collection>Aerospace Database</collection><collection>SciTech Premium Collection</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ProQuest Science Journals</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</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 Basic</collection><jtitle>Solar system research</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kuskov, O. L.</au><au>Kronrod, E. V.</au><au>Kronrod, V. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition</atitle><jtitle>Solar system research</jtitle><stitle>Sol Syst Res</stitle><date>2018-11-01</date><risdate>2018</risdate><volume>52</volume><issue>6</issue><spage>467</spage><epage>479</epage><pages>467-479</pages><issn>0038-0946</issn><eissn>1608-3423</eissn><abstract>The variations of the bulk composition of the silicate Moon (crust + mantle = Bulk Silicate Moon, BSM) depending on the thermal state are explored based on the joint inversion of gravitational, seismic, and petrologic data within the Na
2
O–TiO
2
–CaO–FeO–MgO–Al
2
O
3
–SiO
2
system. The mantle bulk temperature
T
mean
determining the mineral composition and physical properties of the Moon is adopted as the integral characteristic of thermal state. By parameter
T
mean
, all thermal models of the Moon can be conventionally broken down into the “cold” with
T
mean
~ 690–860°C and the “hot” with
T
mean
~ 925–1075°C. The estimations of refractory oxide abundance in lunar rocks depending on the thermal state are included in two different groups. Cold models of BSM are comparable by the bulk content of Al
2
O
3
~ 3.0–4.6 wt % to those for the silicate Earth (Bulk Silicate Earth, BSE), while hot models of BSM are significantly enriched with Al
2
O
3
~ 5.1–7.3 wt % (Al
2
O
3
~ 1.2–1.7 × BSE) as compared with BSE. On the contrary, independent of the temperature distribution, both types of BSM models are characterized by nearly constant values of bulk concentrations of FeO ~ 12–13 wt % and magnesian number MG# 80–81.5 (MG# = [MgO/(MgO + FeO) × 100]), which differ markedly from those for BSE (FeO ~ 8% and MG# 89). It means that for all possible temperature distributions, the silicate fraction of the Moon is FeO-enriched and MgO-depleted in relation to BSE. These arguments discard the possibility of the Moon’s formation out of the material of the Earth’s primitive mantle. In spite of the almost complete coincidence of the isotopic systems, this apparently undeniable fact has no adequate explanation in the existing canonical models of the Moon’s origin and should result in additional constraints on the dynamic processes in models of the formation of the Earth–Moon system. However, the problem of the similarity of and/or difference between compositions of the Moon and the Earth regarding the abundance of refractory elements, which is very important for the geochemistry of the Moon and the Earth’s mantle, remains unresolved and requires further study.</abstract><cop>Moscow</cop><pub>Pleiades Publishing</pub><doi>10.1134/S0038094618060047</doi><tpages>13</tpages></addata></record> |
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subjects | Abundance Aluminum oxide Astronomy Astrophysics and Astroparticles Astrophysics and Cosmology Cold Composition Constraint modelling Crystallization Earth Earth mantle Geochemistry Lunar rocks Magnesium oxide Mineral composition Moon Observations and Techniques Physical properties Physics Physics and Astronomy Planetology Seismic surveys Silicon dioxide Solar system Temperature distribution Thermal analysis Thermal models Titanium dioxide |
title | Geochemical Constraints on the Cold and Hot Models of the Moon’s Interior: 1–Bulk Composition |
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