Equations of state of clino- and orthoenstatite and phase relations in the MgSiO3 system at pressures up to 12 GPa and high temperatures

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作者
Tatiana S. Sokolova
Peter I. Dorogokupets
Alena I. Filippova
机构
[1] Institute of the Earth’s Crust,
[2] SB RAS,undefined
[3] Institute of Earthquake Prediction Theory and Mathematical Geophysics,undefined
[4] RAS,undefined
[5] Pushkov Institute of Terrestrial Magnetism,undefined
[6] Ionosphere and Radio Wave Propagation,undefined
[7] RAS,undefined
来源
Physics and Chemistry of Minerals | 2022年 / 49卷
关键词
Equation of state; Thermodynamics; Pyroxene; Clinoenstatite; Orthoenstatite; Mantle;
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摘要
The equations of state of MgSiO3-pyroxenes (low-pressure clinoenstatite, orthoenstatite and high-pressure clinoenstatite) are constructed using a thermodynamic model based on the Helmholtz free energy and optimization of known experimental measurements and calculated data for these minerals. The obtained equations of state allow us to calculate a full set of thermodynamic and thermoelastic properties as depending on T–P or T–V parameters. We offer open working MS Excel spreadsheets for calculations, which are a convenient tool for solving various user’s tasks. The phase relations in the MgSiO3 system are calculated based on the estimated Gibbs energy for studied MgSiO3-pyroxenes and clarify other calculated data at pressures up to 12 GPa and temperatures up to 2000 K. The obtained orthoenstatite → high-pressure clinoenstatite phase boundary corresponds to the following equation P(GPa) = 0.0021 × T(K) + 4.2. The triple point of equilibrium is determined at 1100 K and 6.5 GPa. Isotropic compressional (P) and shear (S) wave velocities of orthoenstatite and high-pressure clinoenstatite at different pressures are calculated based on the obtained equations of state. The calculated jumps of P- and S-wave velocities of orthoenstatite → high-pressure clinoenstatite phase transition at a pressure of ~ 9 GPa are 0.7 and 5.1%, respectively. The calculated jump of the density of this phase transition at a pressure of 8 GPa, which corresponds to the depth of ~ 250 km, is 2.9%. These results are used to discuss the location of the seismic X-discontinuity at the depths of 250–340 km, which is associated with phase boundaries in enstatite.
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[1]  
Agrusta R(2014)The effect of metastable pyroxene on the slab dynamics Geophys Res Lett 41 8800-8808
[2]  
Van Hunen J(2009)Orthoenstatite/clinoenstatite phase transformation in MgSiO J Geophys Res 28 129-141
[3]  
Goes S(1987) at high-pressure and high-temperature determined by in situ X-ray diffraction: Implications for nature of the X discontinuity Appl Mechan Techn Phys 99 19777-19783
[4]  
Akashi A(1994)Isotherms and Gruneisen functions of 25 metals J Geophys Res 358 322-324
[5]  
Nishihara Y(1992)Equations of state and thermodynamic properties of enstatite pyroxenes Nature 29 1249-1252
[6]  
Takahashi E(2002)Stability of high-density clinoenstatite at upper-mantle pressures Geophys Res Lett 225 295-304
[7]  
Nakajima Y(2004)A systematic search for mantle discontinuities using SS-precursors Earth Planet Sci Lett 410 1091-1095
[8]  
Tange Y(2006)The nature of the Lehmann discontinuity from its seismological Clapeyron slopes Dokl Earth Sci 27 431-446
[9]  
Funakoshi K(2007)Equations of state of Al, Au, Cu, Pt, Ta, and W and revised ruby pressure scale High Press Res 75 172-189
[10]  
Al’tshuler LV(2007)Equations of state of MgO, Au, Pt, NaCl-B1, and NaCl-B2: internally consistent high-temperature pressure scales Phys Rev B 56 459-476