Partition of Ti between quartz and silicate melt. Reply to: Comment on Zhang et al., “Ti-in-quartz thermobarometry and TiO2 solubility in rhyolitic melts: New experiments and parametrization”

2021 ◽  
Vol 561 ◽  
pp. 116846
Author(s):  
Chao Zhang ◽  
Xiaoyan Li ◽  
Renat R. Almeev ◽  
Ingo Horn ◽  
Harald Behrens ◽  
...  
Keyword(s):  
Author(s):  
N. S. Aryaeva ◽  
E. V. Koptev-Dvornikov ◽  
D. A. Bychkov

A system of equations of thermobarometer for magnetite-silicate melt equilibrium was obtained by method of multidimensional statistics of 93 experimental data of a magnetite solubility in basaltic melts. Equations reproduce experimental data in a wide range of basalt compositions, temperatures and pressures with small errors. Verification of thermobarometers showed the maximum error in liquidus temperature reproducing does not exceed ±7 °C. The level of cumulative magnetite appearance in the vertical structure of Tsypringa, Kivakka, Burakovsky intrusions predicted with errors from ±10 to ±50 m.


2021 ◽  
pp. 116773
Author(s):  
Zhe Wang ◽  
Shuheng Huang ◽  
Yue Yu ◽  
Guanghua Wen ◽  
Ping Tang ◽  
...  

2021 ◽  
Vol 573 ◽  
pp. 120192
Author(s):  
Fabien Bernadou ◽  
Fabrice Gaillard ◽  
Evelyn Füri ◽  
Yves Marrocchi ◽  
Aneta Slodczyk

Author(s):  
Eleanor R. MARE ◽  
Hugh St.C. O'NEILL ◽  
Andrew J. BERRY ◽  
Corinne FRIGO ◽  
Chris J. GLOVER

Author(s):  
Carl B Agee

Hydrous silicate melts appear to have greater compressibility relative to anhydrous melts of the same composition at low pressures (<2 GPa); however, at higher pressures, this difference is greatly reduced and becomes very small at pressures above 5 GPa. This implies that the pressure effect on the partial molar volume of water in silicate melt is highly dependent on pressure regime. Thus, H 2 O can be thought of as the most compressible ‘liquid oxide’ component in silicate melt at low pressure, but at high pressure its compressibility resembles that of other liquid oxide components. A best-fit curve to the data on from various studies allows calculation of hydrous melt compression curves relevant to high-pressure planetary differentiation. From these compression curves, crystal–liquid density crossovers are predicted for the mantles of the Earth and Mars. For the Earth, trapped dense hydrous melts may reside atop the 410 km discontinuity, and, although not required to be hydrous, atop the core–mantle boundary (CMB), in accord with seismic observations of low-velocity zones in these regions. For Mars, a density crossover at the base of the upper mantle is predicted, which would produce a low-velocity zone at a depth of approximately 1200 km. If perovskite is stable at the base of the Martian mantle, then density crossovers or trapped dense hydrous melts are unlikely to reside there, and long-lived, melt-induced, low-velocity regions atop the CMB are not predicted.


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