journal article·2011-03

The thermodynamics of several elements at high pressure

A. Karbasi, S.K. Saxena, R. Hrubiak

Calphad· Volume 35· Issue 1
Publisher page

Abstract

Abstract We have used the CALPHAD-compatible equation of state (EOS) based on the explicit Gibbs free energy concept for the solid state of ten important elements: V, Nb, Ta, Mo, W (groups VB and VIB), Pd, Pt (group VIIIB) and Cu, Ag and Au (group IB). The new formulation uses SGTE data for ambient pressure and converges to the quasi-harmonic model at the limit of extreme pressure to calculate the Gibbs free energy as a function of pressure and temperature. The model is based on the available pressure–volume–temperature ( P V T ) data on the elements and can be usefully extrapolated to extreme pressures. When compared to shock wave data, the modeled EOS holds well, but the fit is not totally satisfactory in the ultrahigh-pressure range. A great advantage of this formulation is that it can be used to calculate thermodynamic properties such as the heat capacity and entropy at very high temperatures and pressures.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: High-pressure geophysics and materials · Energetic Materials and Combustion · Chemical Thermodynamics and Molecular Structure

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (100+)

Show source-provided references
1. Lukas · 2007
2. Explicit Gibbs free energy equation of state applied to the carbon phase diagram10.1103/PhysRevB.61.8734 ↗
3. The representation of thermodynamic properties at high pressures10.1016/0022-3697(85)90082-4 ↗
4. A universal equation of state for solids10.1088/0022-3719/19/20/001 ↗
5. Universal features of the equation of state of solids10.1088/0953-8984/1/11/002 ↗
6. Earth mineralogical model: Gibbs free energy minimization computation in the system MgO–FeO–SiO210.1016/0016-7037(96)00096-8 ↗
7. Thermochemical and pressure–volume–temperature systematics of data on solids, examples: tungsten and MgO10.1007/BF00209225 ↗
8. Anderson · 1995
9. A realistic equation of state for solids. The high pressure and high temperature thermodynamic properties of MGO10.1016/S0364-5916(00)00019-5 ↗
10. Application of CALPHAD to high pressures10.1016/j.calphad.2006.12.008 ↗
11. Explicit Gibbs free energy equation of state for solids10.1016/j.jpcs.2008.01.019 ↗
12. Implementation of a new model for pressure dependence of condensed phases in Thermo-Calc10.1016/j.calphad.2005.04.001 ↗
13. A CALPHAD Helmholtz energy approach to calculate thermodynamic and thermophysical properties of fcc Cu
14. Theoretical modeling of molar volume and thermal expansion10.1016/j.actamat.2005.01.049 ↗
15. Assessments of molar volume and thermal expansion for selected bcc, fcc and hcp metallic elements10.1016/j.calphad.2005.05.001 ↗
16. Calculations of thermophysical properties of cubic carbides and nitrides using the Debye–Grüneisen model10.1016/j.actamat.2006.05.054 ↗
17. Thermal expansion of periclase (MgO) and Tungsten (W) to melting temperatures10.1007/s002690050070 ↗
18. Ruby, metals, and MgO as alternative pressure scales: a semiempirical description of shock-wave, ultrasonic, X-ray, and thermochemical data at high temperatures and pressures10.1103/PhysRevB.75.024115 ↗
19. SGTE data for pure elements10.1016/0364-5916(91)90030-N ↗
20. E. Brosh, G. Makov, R.Z. Shneck, Thermodynamic analysis of light-actinide elements. in: Proceedings of the 11th International Symposium on Thermodynamics of Nuclear Materials, vol. 344, issue(1–3), 2005, pp. 36–39.10.1016/j.jnucmat.2005.04.012 ↗
21. Thermodynamic analysis of high-pressure phase equilibria in Fe–Si alloys, implications for the inner-core
22. Intrinsic anharmonicity in equations of state and thermodynamics of solids10.1088/0953-8984/16/8/018 ↗
23. E. Brosh, Personal Communication, 2009.
24. Girifalco · 2000
25. Kittel · 1996
26. ChemSage — a computer program for the calculation of complex chemical equilibria10.1007/BF02670272 ↗
27. Miniaturization techniques for obtaining static pressures comparable to the pressure at the center of the earth: X-ray diffraction at 416 GPa10.1063/1.1141509 ↗
28. Equation of state of Tantalum to 174 GPa10.1103/PhysRevB.59.8526 ↗
29. High-pressure equation of state for Nb with a helium-pressure medium: powder X-ray diffraction experiments10.1103/PhysRevB.73.224119 ↗
30. Structural phase transition of vanadium at 69 GPa10.1103/PhysRevLett.98.085502 ↗
31. Structural phase transitions in Vanadium under high pressure10.1209/0295-5075/81/37003 ↗
32. Ultrahigh-pressure structural phase transitions in Cr, Mo, and W10.1103/PhysRevB.45.2004 ↗
33. The heat capacities of vanadium, vanadium trioxide, vanadium tetroxide and vanadium pentoxide at low temperatures 110.1021/ja01295a006 ↗
34. Heat capacity of reference materials: Cu and W10.1063/1.555728 ↗
35. Critical evaluation of the thermodynamic properties of Molybdenum10.1007/BF00500269 ↗
36. The heat capacity of tantalum from 80 to 1000 K10.1016/0040-6031(95)02797-1 ↗
37. Elastic constants of single-crystal Mo and W between 77 and 500 K10.1063/1.1728952 ↗
38. Elastic constants of tantalum, tungsten, and molybdenum10.1103/PhysRev.130.1324 ↗
39. Single-crystal elastic properties of Tungsten from 24 to 1800 °C10.1063/1.1709158 ↗
40. Elastic properties of vanadium. I. Temperature dependence of the elastic constants and the thermal expansion10.1103/PhysRevB.3.4100 ↗
41. Elastic constants of niobium–molybdenum alloys in the temperature range −190 to +100 °C10.1063/1.1661712 ↗
42. Elastic properties of tantalum over the temperature range 4300 K10.1063/1.1662772 ↗
43. Elastic constants in Nb–Mo alloys from zero temperature to the melting point: experiment and theory10.1088/0305-4608/11/4/011 ↗
44. High-pressure thermoelasticity of body-centered-cubic tantalum10.1103/PhysRevB.65.064103 ↗
45. The thermal expansion of pure metals. II: molybdenum, palladium, silver, tantalum, tungsten, platinum, and lead10.1103/PhysRev.61.74 ↗
46. High temperature structure and thermal expansion of some metals as determined by X-ray diffraction data. I. Platinum, tantalum, niobium, and molybdenum10.1063/1.1699977 ↗
47. Tantalum structure at elevated temperature
48. High temperature X-ray metallography10.1016/0022-5088(63)90031-6 ↗
49. Lattice constants and thermal expansion of palladium and tungsten up to 878 °C by X-ray method10.1002/pssb.19630031207 ↗
50. Niobium and vanadium crystal structure at high temperature
51. Thermal expansion of Vanadium and Vanadium hydride at low temperature10.1016/0022-5088(70)90023-8 ↗
52. High-temperature thermal expansion of Pt, Ta, Mo and W measured by X-ray diffraction
53. Thermophysical properties of matter, volume 12: thermal expansion
54. Étude du comportement du Niobium sous vide par diffraction des rayons X à haute température10.1016/0022-5088(82)90036-4 ↗
55. The role of defects on thermophysical properties: thermal expansion of V, Nb, Ta, Mo and W10.1016/S0927-796X(98)00011-4 ↗
56. Analysis of thermodynamic properties of Molybdenum and Tungsten at high temperatures10.1103/PhysRevB.44.4332 ↗
57. Statistical mechanics of monatomic liquids10.1103/PhysRevE.56.4179 ↗
58. Melting curve of Molybdenum up to 90 kbar
59. Systematics of transition-metal melting10.1103/PhysRevB.63.132104 ↗
60. Melting of Tantalum at high pressure determined by angle dispersive X-ray diffraction in a double-sided laser-heated diamond-anvil cell10.1088/0953-8984/15/45/003 ↗
61. Comment on ‘theoretical solid and liquid state shock Hugoniots of Al, Ta, Mo and W’10.1088/0953-8984/16/47/032 ↗
62. Melting of aluminum, molybdenum, and the light actinides10.1103/PhysRevB.70.184112 ↗
63. Improving the understanding of the melting behaviour of Mo, Ta, and W at extreme pressures10.1016/j.physb.2004.11.087 ↗
64. Phase behavior of metals at very high PT conditions: a review of recent experimental studies10.1016/j.jpcs.2006.05.031 ↗
65. Melting of transition metals at high pressure and the influence of liquid frustration: the late metals Cu, Ni, and Fe10.1103/PhysRevB.76.184117 ↗
66. X-ray diffraction measurements of Mo melting to 119 GPa and the high pressure phase diagram10.1063/1.3082030 ↗
67. Acoustic velocities and phase transitions in Molybdenum under strong shock compression10.1103/PhysRevLett.62.637 ↗
68. Temperature in Molybdenum at high shock pressure: experiment and theory10.1016/j.physb.2008.04.012 ↗
69. Melting behaviour of Mo by shock wave experiment10.1088/0256-307X/25/8/064 ↗
70. Angular forces and melting in bcc transition metals: a case study of Molybdenum10.1103/PhysRevB.49.12431 ↗
71. High-pressure melting of Molybdenum10.1103/PhysRevLett.92.195701 ↗
72. Quantum-based atomistic simulation of materials properties in transition metals10.1088/0953-8984/14/11/305 ↗
73. On high-pressure melting of Tantalum10.1016/j.physb.2006.05.425 ↗
74. Ab initio melting curve of Molybdenum by the phase coexistence method10.1063/1.2735324 ↗
75. Melting curve and Hugoniot of Molybdenum up to 400 GPa by ab initio simulations10.1088/1742-6596/121/1/012009 ↗
76. Thermal equation of state, and melting and thermoelastic properties of bcc tantalum from molecular dynamics10.1016/j.jpcs.2008.07.009 ↗
77. Ab-initio melting curve and principal Hugoniot of Tantalum10.1088/1742-6596/121/1/012010 ↗
78. Theoretical study of melting curves on Ta, Mo, and W at high pressures10.1016/j.physb.2007.11.027 ↗
79. Theoretical solid and liquid state shock Hugoniots of Al, Ta, Mo and W10.1088/0953-8984/16/28/004 ↗
80. Ab initio study of metastability in refractory metal based systems10.1103/PhysRevLett.83.1621 ↗
81. Specific volume measurements of Cu, Mo, Pd, and Ag and calibration of the ruby R fluorescence pressure gauge from 0.06 to 1 Mbar10.1063/1.325277 ↗
82. Equations of state of six metals above 94 GPa10.1103/PhysRevB.70.094112 ↗
83. Y. Nakamoto, K. Takemura, M. Ishizuka, K. Shimizu, T. Kikegawa (Eds.) Equation of state for vanadium under hydrostatic conditions, in: Joint 20th AIRAPT–43th EHPRG, 2005, Karlsruhe, Germany.
84. K.K. Krupnikov, A.A. Bakanova, M.I. Brazhnik, R.F. Trunin (Eds.), An investigation of the shock compressibility of Titanium, Molybdenum Tantalum, and Iron SPhD, 1963.
85. Equation of state for nineteen metallic elements from shock-wave measurements to two megabars10.1063/1.1735815 ↗
86. The equation of state of solids from shock wave studies
87. Isothermal compression of bcc transition metals to 100 kbar10.1063/1.324325 ↗
88. Marsh · 1980
89. Shock adiabats for metals. New data, statistical analysis and general regularities
90. Shock compression of aluminum, Copper, and Tantalum10.1063/1.329160 ↗
91. Hugoniot measurements for Vanadium10.1063/1.336877 ↗
92. Shock compression of Tungsten and Molybdenum10.1063/1.351203 ↗
93. Problems in shock wave reduced isotherms
94. Equations of state of Al, Au, Cu, Pt, Ta, and W and revised ruby pressure scale
95. The equation of state of Molybdenum at 1400 C10.1063/1.341124 ↗
96. Shock compression of preheated Molybdenum to 300 GPa
97. Lattice dynamics and thermal equation of state of platinum10.1103/PhysRevB.78.024304 ↗
98. Theoretical investigation of the Cu EOS standard10.1016/j.jpcs.2006.05.055 ↗
99. The equation of state of the gold calibration standard10.1063/1.333139 ↗
100. Equation of state of Gold and its application to the phase boundaries near 660 km depth in Earth’s mantle10.1016/S0012-821X(02)00917-2 ↗