Liu hard disk equation of state: Difference between revisions
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m (The definition of alpha was missing a -1. See right below Equation (13) on pp. 5 of Liu's paper.) |
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The '''Liu''' [[Equations of state | equation of state]] for [[hard disks]] (2-dimensional [[hard sphere model | hard spheres]]) is given by Eq. 1 of | The '''Liu''' [[Equations of state | equation of state]] for [[hard disks]] (2-dimensional [[hard sphere model | hard spheres]]) is given by Eq. 1, 9 and 13 of | ||
<ref>[https://arxiv.org/abs/2010.10624]</ref>. | <ref>[https://arxiv.org/abs/2010.10624 Hongqin Liu "Global equation of state and phase transitions of the hard disc systems", arXiv:2010.10624 (2020)]</ref>. | ||
For the stable fluid: | For the stable fluid: | ||
:<math>Z_v = \frac{1 + \eta^2/8 + \eta^ | :<math>Z_v = \frac{1 + \eta^2/8 + \eta^3/18 - 4 \eta^4/21}{(1-\eta)^2} </math> | ||
where the packing fraction is given by <math>\eta = \pi \rho \sigma^2 /4 </math> where <math>\sigma</math> is the diameter of the disks. | where the packing fraction is given by <math>\eta = \pi \rho \sigma^2 /4 </math> where <math>\rho</math> is density and <math>\sigma</math> is the diameter of the disks. | ||
The EoS for the stable fluid, liquid-hexatic transition region and hexatic: | The EoS for the stable fluid, liquid-hexatic transition region and hexatic: | ||
Line 19: | Line 19: | ||
<math>Z_{solid} = \frac{2}{\alpha} + 1.9 + \alpha - 5.2 \alpha^2 + 114.48 \alpha^4</math> | <math>Z_{solid} = \frac{2}{\alpha} + 1.9 + \alpha - 5.2 \alpha^2 + 114.48 \alpha^4</math> | ||
and <math>\alpha = \frac{2}{3^{1/2} \rho \sigma^2} - 1</math> | |||
{| border="1" | |||
|- | |||
| <math>b_1</math> || <math>- 1.04191 * 10^8</math> | |||
|- | |||
| <math>b_2</math>|| <math>2.66813 * 10^8</math> | |||
|- | |||
| <math>m_1</math> || 53 | |||
|- | |||
| <math>m_2</math> || 56 | |||
|- | |||
| <math>\frac{1}{c}</math> || 0.75 | |||
|} | |||
==References== | ==References== |
Latest revision as of 18:53, 28 February 2024
The Liu equation of state for hard disks (2-dimensional hard spheres) is given by Eq. 1, 9 and 13 of [1].
For the stable fluid:
where the packing fraction is given by where is density and is the diameter of the disks.
The EoS for the stable fluid, liquid-hexatic transition region and hexatic:
The global EoS for all phases:
,
,
where:
and
53 | |
56 | |
0.75 |