TY - JOUR
T1 - Thermal equation of state to 33.5 GPa and 1673 K and thermodynamic properties of tungsten
AU - Litasov, Konstantin D.
AU - Gavryushkin, Pavel N.
AU - Dorogokupets, Peter I.
AU - Sharygin, Igor S.
AU - Shatskiy, Anton
AU - Fei, Yingwei
AU - Rashchenko, Sergey V.
AU - Seryotkin, Yury V.
AU - Higo, Yiji
AU - Funakoshi, Kenichi
AU - Ohtani, Eiji
N1 - Funding Information:
We thank the reviewers for critical comments and suggestions and Katherine Crispin for technical corrections. This work was conducted as a part of the Global Center-of-Excellence Program “Global Education and research Center for Earth and Planetary dynamics” at Tohoku University and supported by the Ministry of Education and Science of Russia, Project 14.B37.21.0457, Integration project of Siberian Branch RAS No 97 for 2012-2014 and Russian Foundation for Basic Research (No 12-05-00758-а). Experiments were conducted under SPring-8 general research proposals Nos. 2009A1278, 2009B1327, and 2012B1289.
PY - 2013/4/7
Y1 - 2013/4/7
N2 - A comprehensive P-V-T dataset for bcc-tungsten was obtained for pressures up to 33.5 GPa and temperatures 300-1673 K using MgO and Au pressure scales. The thermodynamic analysis of these data was performed using high-temperature (HT) and Mie-Grüneisen-Debye (MGD) relations combined with the Vinet equations of state (EOS) for room-temperature isotherm and the newly proposed Kunc-Einstein (KE) EOS. The KE EOS allowed calibration of W thermodynamic parameters to the pressures of at least 300 GPa and temperatures up to 4000 K with minor uncertainties (<1% in calculated volume of W). A detailed analysis of room-temperature compression data with Vinet EOS yields V0 = 31.71 ± 0.02 Å3, KT = 308 ± 1 GPa, and KT′ = 4.20 ± 0.05. Estimated thermoelastic parameters for HT include (∂KT/∂T)P = -0.018 ± 0.001 GPa/K and thermal expansion α = a0 + a1T with a0 = 1.35 (±0.04) × 10-5 K-1 and a1 = 0.21 (±0.05) × 10-8 K-2. Fitting to the MGD relation yielded γ0 = 1.81 ± 0.02 and q = 0.71 ± 0.02 with the Debye temperature (θ0,) fixed at 370-405 K. The parameters for KE EOS include two Einstein temperatures, ΘE1o = 314 K and ΘE2o = 168 K, Grüneisen parameter at ambient condition γ0 = 1.67 and infinite compression γ∞ = 0.66, with β = 1.16 (which is a power-mode parameter in the Grüneisen equation), anharmonicity (m = 3.57) and electronic (g = 0.11) equivalents of the Grüneisen parameter, and additional parameters for intrinsic anharmonicity, a0 = 6.2 × 10-5 K-1, and electronic contribution, e0 = 4.04 × 10-5 K-1 to the free energy. Fixed parameters include k = 2 in KE EOS and mE1 = mE 2 = 1.5 in expression for Einstein temperature. Present analysis should represent the best fit of the experimental data for W and can be used for a variety of thermodynamic calculations for W and W-containing systems including phase diagrams, chemical reactions, and electronic structure.
AB - A comprehensive P-V-T dataset for bcc-tungsten was obtained for pressures up to 33.5 GPa and temperatures 300-1673 K using MgO and Au pressure scales. The thermodynamic analysis of these data was performed using high-temperature (HT) and Mie-Grüneisen-Debye (MGD) relations combined with the Vinet equations of state (EOS) for room-temperature isotherm and the newly proposed Kunc-Einstein (KE) EOS. The KE EOS allowed calibration of W thermodynamic parameters to the pressures of at least 300 GPa and temperatures up to 4000 K with minor uncertainties (<1% in calculated volume of W). A detailed analysis of room-temperature compression data with Vinet EOS yields V0 = 31.71 ± 0.02 Å3, KT = 308 ± 1 GPa, and KT′ = 4.20 ± 0.05. Estimated thermoelastic parameters for HT include (∂KT/∂T)P = -0.018 ± 0.001 GPa/K and thermal expansion α = a0 + a1T with a0 = 1.35 (±0.04) × 10-5 K-1 and a1 = 0.21 (±0.05) × 10-8 K-2. Fitting to the MGD relation yielded γ0 = 1.81 ± 0.02 and q = 0.71 ± 0.02 with the Debye temperature (θ0,) fixed at 370-405 K. The parameters for KE EOS include two Einstein temperatures, ΘE1o = 314 K and ΘE2o = 168 K, Grüneisen parameter at ambient condition γ0 = 1.67 and infinite compression γ∞ = 0.66, with β = 1.16 (which is a power-mode parameter in the Grüneisen equation), anharmonicity (m = 3.57) and electronic (g = 0.11) equivalents of the Grüneisen parameter, and additional parameters for intrinsic anharmonicity, a0 = 6.2 × 10-5 K-1, and electronic contribution, e0 = 4.04 × 10-5 K-1 to the free energy. Fixed parameters include k = 2 in KE EOS and mE1 = mE 2 = 1.5 in expression for Einstein temperature. Present analysis should represent the best fit of the experimental data for W and can be used for a variety of thermodynamic calculations for W and W-containing systems including phase diagrams, chemical reactions, and electronic structure.
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U2 - 10.1063/1.4799018
DO - 10.1063/1.4799018
M3 - Article
AN - SCOPUS:84880663091
VL - 113
JO - Journal of Applied Physics
JF - Journal of Applied Physics
SN - 0021-8979
IS - 13
M1 - 133505
ER -