Cell model for quantum fluids. III. Compressional waves in liquid hydrogen

1965 ◽  
Vol 18 (9) ◽  
pp. 1309
Author(s):  
R Chen ◽  
D Henderson ◽  
RD Reed
Keyword(s):  
Shock Wave ◽  
Thermodynamic Properties ◽  
Cell Model ◽  
Liquid Hydrogen ◽  
Quantum Fluids ◽  
Velocity Of Sound ◽  
Compressional Waves ◽  
Quantum Parameter

The velocity of sound is calculated for each of the isotopic forms of liquid hydrogen using the quantum cell model. The velocity of sound increases as the pressure increases and decreases as the temperature increases. Also the reduced velocity of sound decreases as the value of the quantum parameter, Λ*, increases. In addition, the thermodynamic properties of liquid hydrogen compressed by a shock wave are calculated.

Cell Model for Quantum Fluids. II. Thermodynamic Properties of Liquid H2

1964 ◽  
Vol 41 (9) ◽  
pp. 2705-2708 ◽  
Author(s):  
Robert D. Reed ◽  
Douglas Henderson
Keyword(s):  
Thermodynamic Properties ◽  
Cell Model ◽  
Quantum Fluids

Thermodynamic Properties of Liquid Hydrogen Metal

1985 ◽  
Vol 128 (2) ◽  
pp. 467-474 ◽  
Author(s):  
W. Ebeling ◽  
W. Richert
Keyword(s):  
Thermodynamic Properties ◽  
Liquid Hydrogen

A New Theory of Fluids: The 'Tunnel' Model

1960 ◽  
Vol 13 (2) ◽  
pp. 187 ◽  
Author(s):  
JA Barker
Keyword(s):  
Thermodynamic Properties ◽  
Hard Sphere ◽  
Cell Model ◽  
New Method ◽  
Virial Expansion ◽  
Cell Theory ◽  
Hard Sphere Fluid ◽  
Tunnel Model

A new method for calculating the thermodynamic properties of liquids and compressed gases is proposed, based on a model in which lines of molecules move almost one-dimensionally in " tunnels ", the walls of the tunnels being formed by neighbouring lines of molecules. This picture is related to the " cell " model, but it is a disordered picture, as is appropriate in a model for fluids, and the problem of the " communal entropy " which besets the cell model, does not arise. The method is applied to the hard-sphere fluid and the calculated pressure/volume isotherm is in very much better agreement with the expected isotherm than either the cell theory or the superposition theory, and also in rather better agreement than the virial expansion truncated after five terms.

Some thermodynamic properties of liquid hydrogen sulphide and deuterium sulphide

1987 ◽  
Vol 19 (7) ◽  
pp. 703-710 ◽  
Author(s):  
A.G Cubitt ◽  
C Henderson ◽  
L.A.K Staveley ◽  
I.M.A Fonseca ◽  
A.G.M Ferreira ◽  
...  
Keyword(s):  
Thermodynamic Properties ◽  
Hydrogen Sulphide ◽  
Liquid Hydrogen

Velocity of Sound in Liquid Hydrogen

Nature ◽  
1949 ◽  
Vol 163 (4141) ◽  
pp. 399-399 ◽  
Author(s):  
A. VAN ITTERBEEK ◽  
L. VERHAEGEN
Keyword(s):  
Liquid Hydrogen ◽  
Velocity Of Sound

scholarly journals Comparison of the lattice-dynamics and cell-model approximations with Monte-Carlo thermodynamic properties

Physica ◽  
1970 ◽  
Vol 49 (1) ◽  
pp. 61-76 ◽  
Author(s):  
A.C. Holt ◽  
W.G. Hoover ◽  
S.G. Gray ◽  
D.R. Shortle
Keyword(s):  
Monte Carlo ◽  
Thermodynamic Properties ◽  
Lattice Dynamics ◽  
Cell Model

STABILITY AND AMBIGUOUS REPRESENTATION OF SHOCK WAVE DISCONTINUITY IN MEDIA WITH ARBITRARY THERMODYNAMIC PROPERTIES

2009 ◽  
Author(s):  
A. P. Likhachev ◽  
A. V. Konyukhov ◽  
V. E. Fortov ◽  
A. M. Oparin ◽  
S. I. Anisimov ◽  
...  
Keyword(s):  
Shock Wave ◽  
Thermodynamic Properties

Velocity of sound isotherms in liquid krypton and xenon

1968 ◽  
Vol 46 (22) ◽  
pp. 3477-3482 ◽  
Author(s):  
C. C. Lim ◽  
D. H. Bowman ◽  
Ronald A. Aziz
Keyword(s):  
Thermodynamic Properties ◽  
Vapor Pressure ◽  
Experimental Error ◽  
Corresponding States ◽  
Suitable Choice ◽  
Velocity Of Sound ◽  
Molecular Parameters ◽  
Triple Points ◽  
Atomic Radii

The velocity of sound was measured with a precision of 0.1% in liquid krypton and xenon at pressures between the vapor pressure and about 65 atm, from near their triple points to near their critical points.A corresponding states treatment of these measurements and previous results in argon showed that, with a suitable choice of relative molecular parameters (σ,ε), the W*(P*,T*) surfaces were coincident to within the experimental error, except for argon near the critical temperature.The relative values of the effective atomic radii σ obtained from this analysis were somewhat lower than those obtained from other thermodynamic properties.

Sign in / Sign up

Export Citation Format

Share Document