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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

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in Cooperation with on an Cooperation-Score of 37%

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Publications (1/1 displayed)

  • 2023Quenching of basaltic melts by volatile exsolution1citations

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Münker, Carsten
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Kronz, Andreas
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Fonseca, Raúl O. C.
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Cieszynski, Hanna
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2023

Co-Authors (by relevance)

  • Münker, Carsten
  • Kronz, Andreas
  • Fonseca, Raúl O. C.
  • Cieszynski, Hanna
  • Wirth, Richard
  • Wombacher, Frank
  • Roddatis, Vladimir
  • Friedrich, Hans-Henning
  • Schreiber, Anja
  • Pakulla, Josua
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article

Quenching of basaltic melts by volatile exsolution

  • Münker, Carsten
  • Kronz, Andreas
  • Fonseca, Raúl O. C.
  • Cieszynski, Hanna
  • Wirth, Richard
  • Wombacher, Frank
  • Roddatis, Vladimir
  • Friedrich, Hans-Henning
  • Schreiber, Anja
  • Ballhaus, Chris
  • Pakulla, Josua
Abstract

<jats:title>Abstract</jats:title><jats:p>Normally, volatiles in silicate melts are ephemeral components that escape as gases when the melt reaches fluid saturation. When fluid saturation occurs at elevated pressure, magmatic fluids may have large amounts of oxide solute dissolved, are less volatile, and may resemble viscous gels. In Cyprus we have the rare case that solutes of a magmatic fluid coexist with H<jats:sub>2</jats:sub>O saturated basaltic to boninitic glasses. Quenching of the melts and fluid solutes was induced by fluid segregation. When the fluids exsolved, the liquidus temperature was raised and the melts were left supercooled, while the system temperature remained ± constant. Quenching rates deduced from the morphologies and compositions of quench crystals were high. We analyzed coexisting glasses and fluid solutes for major and trace elements. The fluid mobile trace elements (Rb, K, Pb, Sr) are enriched in both the glasses and fluid solutes. Both endmembers (melt and fluid) have a common parentage and originated within a hydrous mantle source. The glasses have 2.5 ± 0.25 wt.% H<jats:sub>2</jats:sub>O and record residual H<jats:sub>2</jats:sub>O contents left after fluid exsolution was completed. Water contents in glasses correspond to an H<jats:sub>2</jats:sub>O partial pressure (pH<jats:sub>2</jats:sub>O) of 65 ± 10 MPa and an emplacement depth on the seafloor of 6500 ± 1000 m, provided equilibrium was reached between the pH<jats:sub>2</jats:sub>O imposed by the melts and the seawater column. Following fluid exsolution, the degree of supercooling ∆T of the melts relative to the dry MgO-in-melt liquidus temperature was  – 65 ± 10 °C. The cooling rate ∆T/t at the time of crystallization of dendritic clinopyroxene crystals can be semi-quantified from the distribution of Al<jats:sub>2</jats:sub>O<jats:sub>3</jats:sub> between metastable clinopyroxene dendrites and melt, to at least  – 50 °C h<jats:sup>−1</jats:sup>. Toward the end of the article we speculate if other cases exist where quenching was triggered by fluid exsolution. A possible example are spinifex textures deep inside komatiite flows where quenching rates by conductive cooling did not exceed 0.3 to 1 °C h<jats:sup>−1</jats:sup>. Our proposition assumes that many spinifex-textured komatiites were hydrous, that they contained H<jats:sub>2</jats:sub>O in quantities sufficient to reach fluid saturation at emplacement pressure, and that spinifex textures formed as a result of supersaturation by fluid loss.</jats:p>

Topics
  • melt
  • glass
  • glass
  • laser emission spectroscopy
  • texture
  • crystallization
  • quenching
  • trace element