Thermodynamic Properties of a Simple Hard‐Core System

1966 ◽  
Vol 45 (10) ◽  
pp. 3649-3659 ◽  
Author(s):  
William G. Hoover ◽  
Francis H. Ree
1985 ◽  
Vol 110 (5) ◽  
pp. 246-248 ◽  
Author(s):  
Anthony D. Klemm

1966 ◽  
Vol 44 (5) ◽  
pp. 1037-1046 ◽  
Author(s):  
R. J. Hosking ◽  
J. H. Blackwell

The hard-core pinch configuration with azimuthal equilibrium magnetic field only is considered. Provided finite conductivity is included, unstable axisymmetric modes are found. These instabilities are apparently due to nonlocalized plasma diffusion across the magnetic flux lines. On the laboratory scale, the growth rates do not appear to be significant, when the material of the conducting shell is mercury. For a hydrogen plasma shell, however, it appears that the growth rates may be of practical importance. It is found that the ratio of the current in the shell to the hard-core current has a significant effect on the "spectrum" of instabilities. This effect in part accounts for the observed relative stability of the hard-core system when there is no axial equilibrium magnetic field.


1990 ◽  
Vol 8 (4) ◽  
pp. 753-762 ◽  
Author(s):  
Torsten Kahlbaum ◽  
Andreas Förster

We present a theoretical approach to the thermodynamic properties of nonideal plasmas consisting of neutral atoms, multiply charged ions, and free electrons. Starting with the free energy, we describe the ionization equilibrium of this system by a coupled set of mass action laws (Saha equations). Our model of interaction takes into account Coulomb forces between all charged particles and hard-core forces between all heavy particles and the electrons. The influence of multiple ionization and different interaction parts on plasma composition, mean charge, and equation of state is discussed for xenon. Finally, we show the potential occurrence of the plasma phase transition.


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