Vega equation of state for hard ellipsoids

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The Vega equation of state for an isotropic fluid of hard (biaxial) ellipsoids is given by (Ref. 1 Eq. 20):


Z = 1+B_2^*y + B_3^*y^2 + B_4^*y^3 + B_5^*y^4  
    + \frac{B_2}{4} \left( \frac{1+y+y^2-y^3}{(1-y)^3} 
    -1  -4y -10y^2 -18.3648y^3 - 28.2245y^4 \right)

where Z is the compressibility factor and y is the volume fraction, given by y = ρV where ρ is the number density. The virial coefficients are given by the fits

B_3^* =  10 + 13.094756 \alpha'  - 2.073909\tau' + 4.096689 \alpha'^2 
        +  2.325342\tau'^2 - 5.791266\alpha' \tau',


B_4^* = 18.3648 + 27.714434\alpha' - 10.2046\tau' +  11.142963\alpha'^2 
        + 8.634491\tau'^2 - 28.279451\alpha' \tau' 
        -  17.190946\alpha'^2 \tau' + 24.188979\alpha' \tau'^2 
        + 0.74674\alpha'^3 - 9.455150\tau'^3,

and

B_5^* = 28.2245 + 21.288105\alpha' + 4.525788\tau' +  36.032793\alpha'^2 
        + 59.0098\tau'^2 - 118.407497\alpha' \tau' 
        +  24.164622\alpha'^2 \tau' + 139.766174\alpha' \tau'^2 
        - 50.490244\alpha'^3 - 120.995139\tau'^3 + 12.624655\alpha'^3\tau',

where

B_n^*= B_n/V^{n-1},


\tau' = \frac{4 \pi R^2}{S} -1,

and

\alpha' = \frac{RS}{3V}-1.

where V is the volume, S, the surface area, and R the mean radius of curvature.

For B2 see the page "Second virial coefficient".

[edit] References

  1. Carlos Vega "Virial coefficients and equation of state of hard ellipsoids", Molecular Physics 92 pp. 651-665 (1997)
  2. Carl McBride and Enrique Lomba "Hard biaxial ellipsoids revisited: Numerical results", Fluid Phase Equilibria (2007)
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