Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle
Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We perfor...
Ausführliche Beschreibung
Autor*in: |
Davis, Fred A. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
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2021 |
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Anmerkung: |
© This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 |
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Übergeordnetes Werk: |
Enthalten in: Contributions to mineralogy and petrology - Berlin : Springer, 1947, 176(2021), 9 vom: 12. Aug. |
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Übergeordnetes Werk: |
volume:176 ; year:2021 ; number:9 ; day:12 ; month:08 |
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DOI / URN: |
10.1007/s00410-021-01823-3 |
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Katalog-ID: |
SPR044814178 |
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245 | 1 | 0 | |a Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
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520 | |a Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. | ||
650 | 4 | |a MORB |7 (dpeaa)DE-He213 | |
650 | 4 | |a Oxygen fugacity |7 (dpeaa)DE-He213 | |
650 | 4 | |a Experimental petrology |7 (dpeaa)DE-He213 | |
650 | 4 | |a Mantle petrology |7 (dpeaa)DE-He213 | |
700 | 1 | |a Cottrell, Elizabeth |4 aut | |
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10.1007/s00410-021-01823-3 doi (DE-627)SPR044814178 (SPR)s00410-021-01823-3-e DE-627 ger DE-627 rakwb eng Davis, Fred A. verfasserin (orcid)0000-0002-5222-6330 aut Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 Cottrell, Elizabeth aut Enthalten in Contributions to mineralogy and petrology Berlin : Springer, 1947 176(2021), 9 vom: 12. Aug. (DE-627)25372208X (DE-600)1458979-5 1432-0967 nnns volume:176 year:2021 number:9 day:12 month:08 https://dx.doi.org/10.1007/s00410-021-01823-3 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 176 2021 9 12 08 |
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10.1007/s00410-021-01823-3 doi (DE-627)SPR044814178 (SPR)s00410-021-01823-3-e DE-627 ger DE-627 rakwb eng Davis, Fred A. verfasserin (orcid)0000-0002-5222-6330 aut Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 Cottrell, Elizabeth aut Enthalten in Contributions to mineralogy and petrology Berlin : Springer, 1947 176(2021), 9 vom: 12. Aug. (DE-627)25372208X (DE-600)1458979-5 1432-0967 nnns volume:176 year:2021 number:9 day:12 month:08 https://dx.doi.org/10.1007/s00410-021-01823-3 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 176 2021 9 12 08 |
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10.1007/s00410-021-01823-3 doi (DE-627)SPR044814178 (SPR)s00410-021-01823-3-e DE-627 ger DE-627 rakwb eng Davis, Fred A. verfasserin (orcid)0000-0002-5222-6330 aut Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 Cottrell, Elizabeth aut Enthalten in Contributions to mineralogy and petrology Berlin : Springer, 1947 176(2021), 9 vom: 12. Aug. (DE-627)25372208X (DE-600)1458979-5 1432-0967 nnns volume:176 year:2021 number:9 day:12 month:08 https://dx.doi.org/10.1007/s00410-021-01823-3 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 176 2021 9 12 08 |
allfieldsGer |
10.1007/s00410-021-01823-3 doi (DE-627)SPR044814178 (SPR)s00410-021-01823-3-e DE-627 ger DE-627 rakwb eng Davis, Fred A. verfasserin (orcid)0000-0002-5222-6330 aut Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 Cottrell, Elizabeth aut Enthalten in Contributions to mineralogy and petrology Berlin : Springer, 1947 176(2021), 9 vom: 12. Aug. (DE-627)25372208X (DE-600)1458979-5 1432-0967 nnns volume:176 year:2021 number:9 day:12 month:08 https://dx.doi.org/10.1007/s00410-021-01823-3 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 176 2021 9 12 08 |
allfieldsSound |
10.1007/s00410-021-01823-3 doi (DE-627)SPR044814178 (SPR)s00410-021-01823-3-e DE-627 ger DE-627 rakwb eng Davis, Fred A. verfasserin (orcid)0000-0002-5222-6330 aut Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 Cottrell, Elizabeth aut Enthalten in Contributions to mineralogy and petrology Berlin : Springer, 1947 176(2021), 9 vom: 12. Aug. (DE-627)25372208X (DE-600)1458979-5 1432-0967 nnns volume:176 year:2021 number:9 day:12 month:08 https://dx.doi.org/10.1007/s00410-021-01823-3 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_381 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 176 2021 9 12 08 |
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Enthalten in Contributions to mineralogy and petrology 176(2021), 9 vom: 12. Aug. volume:176 year:2021 number:9 day:12 month:08 |
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Enthalten in Contributions to mineralogy and petrology 176(2021), 9 vom: 12. Aug. volume:176 year:2021 number:9 day:12 month:08 |
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Contributions to mineralogy and petrology |
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Davis, Fred A. @@aut@@ Cottrell, Elizabeth @@aut@@ |
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We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. 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|
author |
Davis, Fred A. |
spellingShingle |
Davis, Fred A. misc MORB misc Oxygen fugacity misc Experimental petrology misc Mantle petrology Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
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Davis, Fred A. |
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1432-0967 |
topic_title |
Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle MORB (dpeaa)DE-He213 Oxygen fugacity (dpeaa)DE-He213 Experimental petrology (dpeaa)DE-He213 Mantle petrology (dpeaa)DE-He213 |
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misc MORB misc Oxygen fugacity misc Experimental petrology misc Mantle petrology |
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misc MORB misc Oxygen fugacity misc Experimental petrology misc Mantle petrology |
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misc MORB misc Oxygen fugacity misc Experimental petrology misc Mantle petrology |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Contributions to mineralogy and petrology |
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title |
Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
ctrlnum |
(DE-627)SPR044814178 (SPR)s00410-021-01823-3-e |
title_full |
Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
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Davis, Fred A. |
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Contributions to mineralogy and petrology |
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Contributions to mineralogy and petrology |
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eng |
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2021 |
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Davis, Fred A. Cottrell, Elizabeth |
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176 |
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Elektronische Aufsätze |
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Davis, Fred A. |
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10.1007/s00410-021-01823-3 |
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(ORCID)0000-0002-5222-6330 |
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(orcid)0000-0002-5222-6330 |
title_sort |
partitioning of $ fe_{2} %$ o_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
title_auth |
Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
abstract |
Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 |
abstractGer |
Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 |
abstract_unstemmed |
Abstract Basalts and peridotites from mid-ocean ridges record fO2 near the quartz-fayalite-magnetite buffer (QFM), but peridotite partial melting experiments have mostly been performed in graphite capsules (~ QFM-3), precluding evaluation of ferric iron’s behavior during basalt generation. We performed experiments at 1.5 GPa, 1350–1400 °C, and fO2 from about QFM-3 to QFM+3 to investigate the anhydrous partitioning behavior of $ Fe_{2} %$ O_{3} $ between silicate melts and coexisting peridotite mineral phases. We find spinel/melt partitioning of $ Fe_{2} %$ O_{3} $ (%${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$) increases as spinel $ Fe_{2} %$ O_{3} $ concentrations increase, independent of increases in fO2, and decreases with temperature, which is consistent with new and previous experiments at 0.1 MPa. We find %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ = 0.63 ± 0.10 and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{cpx}/\mathrm{melt}}%$ = 0.78 ± 0.30. MORB $ Fe_{2} %$ O_{3} $ and $ Na_{2} $O concentrations are consistent with a modeled MORB source with $ Fe_{2} %$ O_{3} $ = 0.48 ± 0.03 wt% ($ Fe^{3+} $/ΣFe = 0.053 ± 0.003) at potential temperatures (TP) from 1320 to 1440 °C. The temperature-dependence of the %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{spl}/\mathrm{melt}}%$ function alone allows ~ 40% of the variation in MORB compositions. If we allow %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ and %${D}_{\mathrm{Fe}2\mathrm{O}3}^{\mathrm{opx}/\mathrm{melt}}%$ to also vary with temperature by tying them to spinel $ Fe_{2} %$ O_{3} $ through intermineral partitioning, then all the MORB data are within error of the model. Our model $ Fe_{2} %$ O_{3} $ concentration for the MORB source would require that the convecting mantle be more oxidized at a given depth than recorded by continental mantle xenoliths. Our result is supported by thermodynamic models of mantle with $ Fe^{3+} $/ΣFe = 0.03 that predict fO2 of ~ QFM-1 near the garnet-spinel transition, which is inconsistent with fO2 of MORB. Our results support previous suggestions that redox melting may occur between 200 and 250 km depth. © This is a U.S. government work and not under copyright protection in the U.S.; foreign copyright protection may apply 2021 |
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container_issue |
9 |
title_short |
Partitioning of $ Fe_{2} %$ O_{3} $ in peridotite partial melting experiments over a range of oxygen fugacities elucidates ferric iron systematics in mid-ocean ridge basalts and ferric iron content of the upper mantle |
url |
https://dx.doi.org/10.1007/s00410-021-01823-3 |
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author2 |
Cottrell, Elizabeth |
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Cottrell, Elizabeth |
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doi_str |
10.1007/s00410-021-01823-3 |
up_date |
2024-07-04T02:26:33.817Z |
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|
score |
7.397867 |