Equation of State of Nickel in WDM Region

Results of theoretical calculations and experimental measurements of the equation of state (EOS) in the region of warm dense matter (WDM) are discussed and applied to nickel. The thermodynamic properties of nickel and its phase diagram are calculated with the use of multi‐phase EOS model. Theoretical calculations of thermodynamic properties of the solid, liquid, and plasma phases, and of the critical point, are compared with results of experiments. The analysis deals with thermodynamic properties of solid nickel at T = 0 and 298 K from different band–structure theories, static compression experiments in diamond anvil cells, and the information obtained in shock‐wave experiments. Thermodynamic data in the liquid and plasma states, resulting from traditional thermophysical measurements, ”exploding wire” experiments, and evaluations of the critical point are presented. Numerous shock‐wave experiments for nickel have been done to measure shock adiabats of crystal and porous samples and release isentropes. These data are analyzed in a self‐consistent manner together with all other available data at high pressure. (© 2016 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)

[1]  E. Apfelbaum The calculation of thermophysical properties of nickel plasma , 2015 .

[2]  A. Ramana,et al.  An Orbital‐Free Quantum Hypernetted Chain Model Based Perturbation Theory for Equation of State of Hydrogen and Helium in Warm Dense Regime , 2015 .

[3]  M. W. C. Dharmawardana A Review of Studies on Strongly‐Coupled Coulomb Systems Since the Rise of DFT and SCCS‐1977 , 2014, 1412.6811.

[4]  G. Morard,et al.  The melting curve of Ni to 1 Mbar , 2014 .

[5]  V. Fortov,et al.  Ya B Zeldovich and equation of state problems for matter under extreme conditions , 2014 .

[6]  C. Blancard,et al.  A database for equations of state and resistivities measurements in the warm dense matter regime , 2012 .

[7]  M. Torrent,et al.  Compression curves of transition metals in the Mbar range: Experiments and projector augmented-wave calculations , 2008 .

[8]  I. Lomonosov Multi-phase equation of state for aluminum , 2007 .

[9]  M. Murakami,et al.  Equation of state and optimum compression in inertial fusion energy , 2007 .

[10]  V. N. Korobenko,et al.  Electrical resistivity and equation of state measurements on hot expanded aluminum in the metal-nonmetal transition range , 2007 .

[11]  A. R. Piriz,et al.  Proposal for the study of thermophysical properties of high-energy-density matter using current and future heavy-ion accelerator facilities at GSI Darmstadt. , 2005, Physical review letters.

[12]  R Schmidt,et al.  The CERN Large Hadron Collider as a tool to study high-energy density matter. , 2005, Physical review letters.

[13]  Dmitry Varentsov,et al.  Present and future perspectives for high energy density physics with intense heavy ion and laser beams , 2005 .

[14]  P. Renaudin,et al.  Aluminum equation-of-state data in the warm dense matter regime. , 2003, Physical review letters.

[15]  L. Dubrovinsky,et al.  Whole-cell heater for the diamond anvil cell , 2003 .

[16]  S. Crockett,et al.  Test of a theoretical equation of state for elemental solids and liquids , 2002, cond-mat/0210600.

[17]  Dmitry Varentsov,et al.  Unique capabilities of an intense heavy ion beam as a tool for equation-of-state studies , 2002 .

[18]  G. V. Simakov,et al.  Shock Compression of Porous Aluminum and Nickel at Megabar Pressures , 2001 .

[19]  G. V. Simakov,et al.  Shock compression and isentropic expansion of porous samples of tungsten, nickel, and tin , 2000 .

[20]  G. V. Simakov,et al.  Shock compression and thermodynamics of highly nonideal metallic plasma , 1998 .

[21]  S. Saxena,et al.  Laser-heated diamond anvil cell experiments at high pressure: Melting curve of nickel up to 700 kbar , 1993 .

[22]  M. A. Winkler,et al.  Sound speed and thermophysical properties of liquid iron and nickel. , 1990, Physical review. B, Condensed matter.

[23]  G. R. Gathers Dynamic methods for investigating thermophysical properties of matter at very high temperatures and pressures , 1986 .

[24]  C. Dj New crystalline structures for Si and Ge. , 1985 .

[25]  M. Ross,et al.  Matter under extreme conditions of temperature and pressure , 1985 .

[26]  V. Fortov,et al.  Model equations of state , 1983 .

[27]  A. Jayaraman,et al.  Diamond anvil cell and high-pressure physical investigations , 1983 .

[28]  R. Albers,et al.  Insulating Nickel at a Pressure of 34 TPa , 1982 .

[29]  S. Marsh Lasl Shock Hugoniot Data , 1980 .

[30]  D. Steinberg,et al.  Pressure and temperature derivatives of the isotropic polycrystalline shear modulus for 65 elements , 1974 .

[31]  David A. Young,et al.  Critical Point of Metals from the van der Waals Model , 1971 .

[32]  L. V. Al’tshuler Reviews of Topical Problems: Use of Shock Waves in High-Pressure Physics , 1965 .

[33]  S. P. Marsh,et al.  Equation of State for Nineteen Metallic Elements from Shock‐Wave Measurements to Two Megabars , 1960 .

[34]  R. Mcqueen,et al.  SHOCK-WAVE COMPRESSIONS OF TWENTY-SEVEN METALS. EQUATIONS OF STATE OF METALS , 1957 .