Isobaric VLE data were measured for the acetone-methanol binary system
at 101.32 kPa and for the acetone-methanol-salt system at the same pr
essure at different salt concentrations using a modified Othmer equili
brium still. Both salts investigated in this work, KI and NaI, exhibit
ed a salting-out effect on acetone. The experimental data for the salt
-free system were correlated by Wilson, NRTL and UNIQUAC models. For t
he salt systems, the experimental data were correlated by the electrol
ytic NRTL model of Mock et al. [Mock, B., Evans, L.B. and Chen, C.C.,
1986. AIChE J., 32: 1655-1664], the extended UNIQUAC equation of Sande
r et al. [Sander, B., Fredenslund, A. and Rasmussen, P., 1986. Chem. E
ng. Sci., 41: 1171-1183], and the modified Wilson and NRTL models prop
osed by Tan [Tan, T.C., 1985. AIChe J., 31: 2083-2085; Tan, T.C., 1987
. Chem. Eng. Res. Des., 65: 355-366; Tan, T.C., 1990. Trans. Ind. Eng.
Chem., 68: 93-102]. The results were compared with the data predicted
by the modified Wilson and NRTL models of Tan. The mean absolute devi
ations in vapour-phase mole fraction and bubble points for the salt-fr
ee system were about 0.002 and 0.02, respectively. The mean absolute d
eviations in vapour-phase mole fraction and bubble points for both sal
t systems, over 252 data points, were about 0.004 and 0.21, respective
ly, using the electrolytic NRTL model of Mock et al., 0.009 and 0.44 u
sing the extended UNIQUAC model of Sander et al., 0.024 and 0.38 using
Tan's modified Wilson model, and 0.019 and 0.15 using Tan's modified
NRTL model. Both the modified Wilson and the NRTL models proposed by T
an predict the vapour composition of both salt systems with a mean abs
olute error of about 0.024-0.019, and the bubble points with a mean ab
solute error of about 0.56.