Self-consistent-average-phonon equation of state. II. Comparison with solid-rare-gas experiments

1982 ◽  
Vol 25 (2) ◽  
pp. 1297-1309 ◽  
Author(s):  
A. Paskin ◽  
A. -M. Llois de Kreiner ◽  
K. Shukla ◽  
D. O. Welch ◽  
G. J. Dienes
2012 ◽  
Vol 8 (1) ◽  
pp. 76-80 ◽  
Author(s):  
K. Falk ◽  
S.P. Regan ◽  
J. Vorberger ◽  
M.A. Barrios ◽  
T.R. Boehly ◽  
...  

Polymer ◽  
1991 ◽  
Vol 32 (17) ◽  
pp. 3170-3176 ◽  
Author(s):  
S Saeki ◽  
M Tsubokawa ◽  
J Yamanaka ◽  
T Yamaguchi

1981 ◽  
Vol 24 (2) ◽  
pp. 724-729 ◽  
Author(s):  
K. Shukla ◽  
A. Paskin ◽  
D. O. Welch ◽  
G. J. Dienes

2001 ◽  
Vol 43 (7) ◽  
pp. 1345-1352 ◽  
Author(s):  
E. V. Zarochentsev ◽  
E. P. Troitskaya
Keyword(s):  

2009 ◽  
Vol 64 (1-2) ◽  
pp. 54-58
Author(s):  
Quan Liu

A new isothermal equation of state (EOS) for solids is derived by starting from the theory of lattice potential and using an analytical function for the volume dependence of the short-range force constant. A critical analysis of the isothermal EOSs: Murnaghan EOS, Vinet EOS, and the new EOS derived here, is presented by investigating the pressure-volume data for rare gas solids, metals and minerals. It is found that the results obtained from the new EOS are in good accordance with the corresponding values obtained from the Vinet EOS and with experimental data for all the solids up to very large compressions. On the other hand, the Murnaghan EOS is less successful at high pressure in most cases.


1993 ◽  
Vol 137 ◽  
pp. 307-309 ◽  
Author(s):  
D. Saumon ◽  
G. Chabrier

An improved theory of fluid hydrogen at high density, based on a detailed treatment of inter-particle correlations and a self-consistent treatment of pressure ionization, has become available recently (Chabrier 1990, Saumon and Chabrier 1991, 1992). We present a preliminary comparison between this new EOS (hereatfer SC) and equations of state frequently used in astrophysical contexts, namely: Fontaine, Graboske and Van Horn 1977 (FGVH), Däppen et al. 1988 (MHD) and Magni and Mazzitelli 1979 (MM).The SC theory predicts a first-order phase transition in the region of pressure-ionization (the so-called Plasma Phase Transition, or PPT), between an essentially neutral mixture of atoms and molecules (xe– < 10−2), and a partially ionized plasma (xe– ≈ 50 %), with a critical point located at Pc = 0.614 Mbar, Tc = 15300K and pc = 0.35 g/cm3.


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