Liu hard sphere equation of state: Difference between revisions
Jump to navigation
Jump to search
No edit summary |
Carl McBride (talk | contribs) m (Slight tidy) |
||
Line 1: | Line 1: | ||
Hongqin Liu proposed a correction to the | Hongqin Liu proposed a correction to the [[Carnahan-Starling equation of state]] which improved accuracy by almost two orders of magnitude <ref>[https://arxiv.org/abs/2010.14357 Hongqin Liu "Carnahan Starling type equations of state for stable hard disk and hard sphere fluids", arXiv:2010.14357]</ref>: | ||
: <math> | : <math> | ||
Line 5: | Line 5: | ||
</math> | </math> | ||
The conjugate virial coefficient correlation is given by: | The conjugate [[Virial equation of state | virial coefficient]] correlation is given by: | ||
: <math> | : <math> | ||
Line 11: | Line 11: | ||
</math> | </math> | ||
The excess Helmholtz | The excess [[Helmholtz energy function]] is given by: | ||
: <math> | : <math> | ||
Line 17: | Line 17: | ||
</math> | </math> | ||
The isothermal compressibility is given by: | The isothermal [[compressibility]] is given by: | ||
: <math> | : <math> | ||
Line 28: | Line 28: | ||
\frac{ dZ}{d\eta} = \frac{ 4 + 4\eta - \frac {11}{13} \eta^2 - \frac{52}{13}\eta^3 + \frac {7}{2}\eta^4 - \eta^5 }{(1-\eta)^4 }. | \frac{ dZ}{d\eta} = \frac{ 4 + 4\eta - \frac {11}{13} \eta^2 - \frac{52}{13}\eta^3 + \frac {7}{2}\eta^4 - \eta^5 }{(1-\eta)^4 }. | ||
</math> | </math> | ||
== References == | |||
<references/> | |||
[[Category: Equations of state]] | |||
[[category: hard sphere]] |
Latest revision as of 11:21, 10 November 2020
Hongqin Liu proposed a correction to the Carnahan-Starling equation of state which improved accuracy by almost two orders of magnitude [1]:
The conjugate virial coefficient correlation is given by:
The excess Helmholtz energy function is given by:
The isothermal compressibility is given by:
where