Gibbs Project


CH3OH

Contents


Models
Two models were examined, the H1 model by Haughney et al., J. Phys. Chem., 91, 4934 (1987) and the L1 model by v. Leeuwen et Smit., J. Phys. Chem., 9, 1831 (1995).

H1: CH3: eps/kb(K) = 91.15, sigma(A) = 3.861, q(e) = 0.297, O: eps/kb(K) = 87.94, sigma(A) = 3.083, q(e) = 0.728, H: q(e) = 0.431

L1: CH3: eps/kb(K) = 105.2, sigma(A) = 3.74, q(e) = 0.265, O: eps/kb(K) = 86.5, sigma(A) = 3.030, q(e) = 0.7, H: q(e) = 0.435


Phase envelope/Vapor pressure calculation by virtual volume changes
Several points on the phase envelope of CH3OH for temperatures between 400 K and 500 K were calculated and compared with experimental data and the simulation results of Haughney et al. and v. Leeuwen and Smit. Our results agree with the simulation data of both references within the statistical uncertainties, very good agreement with experimental data is found for the L1 model. The L1 model is also better fit for the vapor pressure calculation.



rho(g/cm3)

T(K)

liquid

vapor

liquid

vapor

liquid

vapor

Gibbs

Haughney et al.

experimental

400

0.597(12)

0.019(5)

0.588(14)

0.014(3)

0.676

0.009

460

0.438(24)

0.055(18)

0.461(11)

0.067(8)

0.577

0.038

Gibbs

v. Leeuwen et al.

experimental

400

0.699(13)

0.008(1)

0.673(12)

0.007(2)

0.676

0.009

450

0.577(13)

0.027(4)

0.601(13)

0.037(13)

0.597

0.030

490

0.488(35)

0.100(7)

0.462(13)

0.094(12)

0.495

0.087


pS(bar)

T(K)

Gibbs

Haughney et al.

experimental

400

15(1)

14(3)

7.703

460

42(6)

46(18)

31.08

T(K)

Gibbs

v. Leeuwen and Smit

experimental

400

7(1)

7(2)

7.703

450

25(4)

37(5)

25.03

490

61(3)

50(26)

54.66


Go to:

Top

Index


Page created by Johannes, August 9th, 1996