Heat Capacity of Na2O2at High Temperatures

1959 ◽  
Vol 63 (9) ◽  
pp. 1505-1506 ◽  
Author(s):  
M. S. Chrasekharaiah ◽  
R. T. Grimley ◽  
John L. Margrave
1978 ◽  
Author(s):  
Richard A. Robie ◽  
B.S. Hemingway ◽  
C.M. Schafer ◽  
J.L. Haas

Silicon ◽  
2018 ◽  
Vol 10 (5) ◽  
pp. 2307-2315
Author(s):  
Boussaid Olfa ◽  
Boussaid Ahlem ◽  
Fnaiech Mustapha

2020 ◽  
Vol 307 ◽  
pp. 112935 ◽  
Author(s):  
Z.I. Zaripov ◽  
A.U. Aetov ◽  
R.R. Nakipov ◽  
V.F. Khairutdinov ◽  
F.M. Gumerov ◽  
...  

1993 ◽  
Vol 201 ◽  
pp. 120-125 ◽  
Author(s):  
Toshihide Tsuji ◽  
Tatsuya Kato ◽  
Keiji Naito

2011 ◽  
Vol 25 (05) ◽  
pp. 333-344 ◽  
Author(s):  
CHENGHUA HU ◽  
FENG WANG ◽  
CHUANHUI XIA ◽  
ZHOU ZHENG ◽  
WEIYI REN

We perform first-principles calculations for fcc-6 LiT in order to study its structure, stability and thermodynamic properties under high temperatures and pressures. We find that melting point of 6 LiT (0 GPa) is about 680 K, and rise with the pressures. Reverse equivalent pressure P r and critical pressure P c of different temperatures are predicted from [Formula: see text] or [Formula: see text], and they are found to increase with temperature. 6 LiT should be stable under the condition of P < 80 GPa and T < 680 K . We also find that pressure and temperature will cause different effect of shear on the {100} and {110} planes. Heat capacity of different pressures increase with temperature and closes to the Dulong–Petit limit at higher temperatures. Debye temperature decreases with temperature, and increases with pressure.


Sign in / Sign up

Export Citation Format

Share Document