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Marcello Campione Università degli Studi di Milano Bicocca, Italy

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Presentation on theme: "Marcello Campione Università degli Studi di Milano Bicocca, Italy"— Presentation transcript:

1 Marcello Campione Università degli Studi di Milano Bicocca, Italy
EGU – Vienna – April 9th 2018 Mantle mineral microcavities filled with aqueous fluids HPHT reactors producing unexpected mineral assemblages Marcello Campione Università degli Studi di Milano Bicocca, Italy

2 Orthopyroxenites – Maowu Ultramafic Complex
Amp + H2O Grt OM 5 µm SEM Interaction of harzburgites and slab-derived silica-rich liquids at the slab-mantle interface Multiphase solid inclusions in garnet P = 4 Gpa T = 800 °C Malaspina et al., EPSL, 2006 Chen et al., LITHOS, 2017 Marcello Campione EGU – Vienna – April 9th 2018 1#9

3 Garnet (pyrope) stability … and Assemblage Stability
Isochemical section (Perple_X, Connolly 2005) Chemography 1 Amp + H2O Grt 3MgO + Al2O3 + 3SiO2 1 2 2 3 3 Marcello Campione EGU – Vienna – April 9th 2018 2#9

4 Garnet (pyrope) stability … and Assemblage Stability
Isochemical section (Perple_X, Connolly 2005) Chemography Amp + H2O Grt 3MgO + Al2O3 + 3SiO2 Py is stable e at T = 800 °C and p  1.7 GPa Py-sp-clin is a stable assemblage (T=800 °C and p4 Gpa) WHAT DIRVES THE SELECTION OF A PY-SP-CLIN ASSEMBLAGE WITHIN THE MICROCAVITY??? Marcello Campione EGU – Vienna – April 9th 2018 3#9

5 Solid-Liquid Interaction – Equilibrated Fluids
Aqueous speciation-solubility code EQ3+ Deep Earth Model (Wolery 1992; Facq et al., 2014; Sverjensky et al., 2014)  Fluid in equilibrium with K-free eclogite (Kessel et al., 2005) SLAB INCLUSION  Fluid in equilibrium with mantle peridotites (Dvir et al., 2011)  Fluid in equilibrium with py-clin-sp assemblage (Fockenberg et al., 2008) MANTLE SLAB FLUIDS ARE SILICA-RICH IF EQUILIBRATED Marcello Campione EGU – Vienna – April 9th 2018 4#9

6 Solid-liquid Interaction – Non-Equilibrated Fluids
A Model of Dissolution-Reprecipitation Campione et al., GPL, 2017 Pyrope congruent dissolution Py(s)  3MgO(aq) + Al2O3(aq) + 3SiO2(aq) m = molality of MgO(aq) a = molality of Al2O3(aq) s = molality of SiO2(aq) M = molality of MgO(aq) A = molality of Al2O3(aq) S = molality of SiO2(aq) Spinel precipitation MgO(aq) + Al2O3(aq)  MgAl2O4(epi) Clinochlore precipitation 10MgO(aq) + 2Al2O3(aq) + 6SiO2(aq) + 8H2O  Mg10Al2[Al2Si6O20](OH)16(s) Marcello Campione EGU – Vienna – April 9th 2018 5#9

7 Solid-liquid Interaction – Non-Equilibrated Fluids
A Model of Dissolution-Reprecipitation Campione et al., GPL, 2017 Pyrope congruent dissolution Py(s)  3MgO(aq) + Al2O3(aq) + 3SiO2(aq) Spinel precipitation MgO(aq) + Al2O3(aq)  MgAl2O4(epi) Clinochlore precipitation 10MgO(aq) + 2Al2O3(aq) + 6SiO2(aq) + 8H2O  Mg10Al2[Al2Si6O20](OH)16(s) 𝑀=𝑚+ 3𝑝 𝑦 − 𝑠 𝑝 −10 𝑐 𝑙 py = moles of dissolved py sp = moles of precipitated sp cl = moles of precipitated clin 1 kg H2O 𝐴=𝑎+ 𝑝 𝑦 − 𝑠 𝑝 −2 𝑐 𝑙 𝑆=𝑠+ 3𝑝 𝑦 −6 𝑐 𝑙 𝐻=56−8 𝑐 𝑙 Marcello Campione EGU – Vienna – April 9th 2018 6#9

8 Solid-liquid Interaction – Non-Equilibrated Fluids
A Model of Dissolution-Reprecipitation Campione et al., GPL, 2017 𝑀=𝑚+ 3𝑝 𝑦 − 𝑠 𝑝 −10 𝑐 𝑙 𝐴=𝑎+ 𝑝 𝑦 − 𝑠 𝑝 −2 𝑐 𝑙 𝑆=𝑠+ 3𝑝 𝑦 −6 𝑐 𝑙 𝐻=56−8 𝑐 𝑙 m = molality of MgO(aq) a = molality of Al2O3(aq) s = molality of SiO2(aq) Solving for py, sp, cl  0 𝑝 𝑦 = 𝑝 𝑦0 − 𝑎 2 − 2𝑠 3 + 𝑚 2 𝑠 𝑝 = 𝑠 𝑝0 +𝑎− 𝑠 3 𝑐 𝑙 = 𝑐 𝑙0 − 𝑎 4 − 𝑠 6 + 𝑚 4 THERE IS NO UPPER LIMIT FOR m Chl INCREASES WITH m WHILE Sp IS CONSTANT A SILICA-RICH FLUID SUPPRESSES THIS DISSOLUTION-REPRECIPITATION MECHANISM!!! Marcello Campione EGU – Vienna – April 9th 2018 7#9

9 Model of Metasomatic Garnet Growth
MANTLE En+Fo+Py MANTLE En+Fo+Py Silica-poor fluid “FILTER” En+Py Silica-rich fluid SLAB Coe+Py+Ky SLAB Coe+Py+Ky MANTLE En+Fo+Py SLAB Coe+Py+Ky Marcello Campione EGU – Vienna – April 9th 2018 8#9

10 Model of Metasomatic Garnet Growth
Retrograde crystallization of hydrous phases Dissolution-reprecipitation of spinel and chlorite in garnet at UHP Aqueous fluid entrapment in garnet Marcello Campione EGU – Vienna – April 9th 2018 9#9


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