Abstract
Abstract. Oxygen fugacity (fO2) is a fundamental variable affecting phase equilibrium in magmas, and in externally heated pressure vessel experiments it is typically controlled by using redox buffer assemblages. However, these do not allow fine enough resolution; for example, most arc magmas fall between the fO2 imposed by the neighboring Ni–NiO and Re–ReO2 buffers and so does the transition of S2− to S6+ in magmas. Here we propose a new method to quantitatively impose fO2 in hydrous high-P–T experiments in molybdenum hafnium carbide (MHC) pressure vessels by admixing small amounts of hydrogen into the Ar pressure medium. The thermodynamic calculation procedure used to determine the initial amount of hydrogen to be loaded to constrain desired fO2 values was verified by CoPd alloy redox sensor experiments to be accurate within ±0.3 log units for the pressure (P) – temperature (T) range of 940–2060 bar and 800–1100 ∘C. As hydrogen can be slowly lost from the pressure medium due to diffusion through the vessel walls at high T, we also determined the hydrogen permeability of the MHC alloy as a function of T. The such-obtained hydrogen permeability equation for the MHC alloy can be used to determine the rate of fO2 increase for any MHC pressure vessel configuration. As the rate of fO2 increase is slow (e.g., 0.36 log units per day in our setup at T= 1000 ∘C), we propose that H2 addition to the Ar pressure medium is an effective way to accurately impose fO2 in many types of experiments conducted in MHC vessels allowing experimentation up to T= 1200 ∘C and P= 300 MPa.
Highlights
High-pressure–temperature experiments have greatly contributed to our present understanding of physical–chemical processes in the Earth’s interior
We present systematic set of experiments to address how precisely f H2 can be controlled in molybdenum hafnium carbide (MHC) pressure vessel experiments
We suggest that as long as the vessels are not exposed to extreme temperatures or allowed to alloy with other materials, the hydrogen permeability values determined here remain applicable to MHC alloy and likely titanium zirconium molybdenum (TZM) alloy
Summary
High-pressure–temperature experiments have greatly contributed to our present understanding of physical–chemical processes in the Earth’s interior. Muan and Osborn (1956), Muan (1958), and Osborn (1959) pointed out the effect of oxygen fugacity (f O2) on the natural course of crystallization and residual liquid compositions in multicomponent oxide melts and iron-bearing mafic magmas This is a consequence of the fact that the Fe2+ / Fe3+ ratio in the melt and mineral phases is a function of f O2 (Botcharnikov et al, 2005; Canil and O’Neill, 1996; Carmichael and Nicholls, 1967; Cottrell and Kelley, 2011; Gaillard et al, 2001; Kilinc et al, 1983; Kress and Carmichael, 1991; Luth et al, 1990; Wilke and Behrens, 1999). Precise control of f O2 is required in high-P –T ex-
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