<>Introduction
Phase
equilibrium calculations of a solid dissolved in a compressed gas, at a
pressure P and a temperature T can be performed using the fundamental equation
of phase equilibria which leads to a simple equation that relates the
solubility y the pressure P, and the temperature T. The equation also contains
other properties such as the sublimation pressure Psub , the molar
volume of the solid Vs and the fugacity coefficient of the solid
component in the high pressure gas fs [1]. Of all these properties involved in the
calculation of the solubility of the solid in the high pressure gas, the
sublimation pressure has received low attention in the literature, although it
is directly related to the solubility. The molar volume does not have a strong
influence on the calculations and the fugacity coefficient fs can be
estimated from an appropriate equation of state and mixing rules. The
sublimation pressure is usually small for common industrially important solids
and in many cases available experimental techniques cannot be used to obtain
accurate values.
In theory, the
calculated sublimation pressures should be independent of the solvent used, but
this statement must be proved. In this article the influence of the type of
solvent in which the solid is dissolved on the calculation of Psub,
is analyzed. For this, the sublimation pressure of anthracene, naphthalene and
phenanthrene in solvents of different nature (carbon dioxide, ethane and
fluoroform), are determined to prove what in theory seems to be clear.
Solubility
Calculations
The theory of solid solubility in a
compressed gas is found in standard books [1, 2]. If subscript 2 stand
for the solid component in the gas-solid mixture, the so-called solubility
equation is:
(1)
Here,
is the sublimation
pressure of the pure solid,
is the solid molar
volume, all at the temperature T and j2 is the fugacity coefficient of solid (2) at the pressure P. The
fugacity coefficient is calculated from standard thermodynamic relations [2].
The
Peng-Robinson equation (PR) [3], with the mixing rules proposed by Wong and Sandler [4], are used as
the thermodynamic model to evaluate the fugacity coefficient j2. The excess Gibbs free energy that appears in the Wong-Sandler
mixing rule (WS) is represented by the van Laar model (VL). Therefore, the
model contains three parameters (the van Laar constants A12 and A21
and the k12 parameter included in the mixing rule). This model is
designed here as PR/WS/VL and the expressions for the
fugacity coefficient can be found elsewhere [1]. The problem is then
reduced here to determine the three parameters of the thermodynamic model and
the sublimation pressure
that appears in the
solubility equation (1), using available high pressure TPy data for gas-solid
systems.
Binary system containing anthracene, napthalene and phenanthrene as solute in various solvents (carbon dioxide, ethane, fluoroform) were considered in the study. The data consisted of 30 isotherms and a total of 381 PTy data points.
<>Results and Discussion The accuracy of the model and the method used to calculate the sublimation pressure is evaluated by considering the deviations between experimental [5-8] and calculated values of the solubility of the solid in the high pressure gas. Literature information indicate that deviations are less than 10% using the PR/WS/VL model [9], deviations that were found of the same order in this study. The Table 1 shows the results obtained using PR/WS/VL model for gas-solid systems considered in this study. The calculated sublimation pressure and the deviations with respect to experimental data are given. For systems which contain naphthalene as solute, the relative deviations vary from -0.22% to 7.5%. For the systems which contain phenanthrene as solute, the relative deviations vary from 0.09% to -6.8% and for systems which contain anthrace as solute, the relative deviations vary from -0.05 % to 7.7%.
Fig. 1 shows sublimation pressure calculated from napthalene for all isotherms with different solvents. The symbols in the Fig. are (*) CO2 for T= 308, 328, 333 and 338 K; and (D) ethane for T= 318 K. The values for fluoroform are not shown in the figure since the isotherms and the calculated values coincide with those of the system naphthalene + CO2 and naphthalene + ethane. In the figure, sublimation pressure is in bar and T in Kelvin. The results shown in Fig. 1 indicate that the proposed method is reliable enough to estimate the sublimation pressure of solids using solubility data of the solid in high pressure gases. The solvent present in the mixture shows to be irrelevant in determining Psub as expected. Table 1: Sublimation pressures of the solid solutes at all temperatures studied and relative deviations between calculated and experimental values. N is the number of experimental data.
|
Naphthalene+ |
T(K) |
N |
Psubx104(bar) |
% ΔPsub |
|
CO2 |
308 |
9 |
2.705 |
7.46 |
|
328 |
16 |
16.060 |
-0.32 |
|
|
333 |
19 |
24.070 |
1.62 |
|
|
338 |
7 |
33.790 |
2.01 |
|
|
Ethane |
308 |
15 |
2.892 |
1.06 |
|
318 |
12 |
7.194 |
-2.39 |
|
|
328 |
14 |
15.900 |
0.68 |
|
|
308 |
6 |
3.090 |
-5.71 |
|
|
318 |
8 |
7.089 |
-0.90 |
|
|
Fluoroform |
308 |
6 |
3.026 |
-3.52 |
|
318 |
6 |
7.099 |
-1.04 |
|
|
328 |
6 |
16.930 |
-5.75 |
|
|
Phenanthrene+ |
|
|
Psubx106(bar) |
|
|
CO2 |
313 |
26 |
0.906 |
0.33 |
|
323 |
30 |
2.677 |
-4.12 |
|
|
333 |
30 |
6.947 |
-1.73 |
|
|
Ethane |
318 |
6 |
1.546 |
-0.32 |
|
328 |
6 |
4.249 |
-0.66 |
|
|
333 |
7 |
6.993 |
-2.40 |
|
|
Fluoroform |
318 |
4 |
1.646 |
-6.81 |
|
328 |
4 |
4.276 |
-1.30 |
|
|
Anthracene+ |
|
|
Psubx107 (bar) |
|
|
CO2 |
323 |
8 |
1.89 |
7.76 |
|
343 |
9 |
19.10 |
-2.59 |
|
|
313 |
30 |
0.61 |
0.16 |
|
|
323 |
30 |
2.05 |
-0.05 |
|
|
333 |
30 |
6.38 |
0.08 |
|
|
Ethane |
308 |
4 |
0.31 |
4.32 |
|
323 |
10 |
2.07 |
-1.02 |
|
|
343 |
7 |
18.60 |
0.10 |
|
|
Fluoroform |
328 |
8 |
3.67 |
-0.60 |
|
343 |
8 |
18.80 |
-0.98 |
Fig. 1: Calculated sublimation pressure of Naphthalene.: (*) CO2 for T= 308, 328, 333 and 338 K; and (D) ethane for T= 318 K. (·) experimental sublimation pressure.
<>Conclusions Sublimation pressure of solid from high pressure solubility data are calculated using genetic algorithms. Based on the results and discussion presented in this study, the following main conclusions are obtained: i) the low deviations between experimental and calculated values of the sublimation pressure show that the thermodynamic model PR/WS/VL is appropriate to model these systems and to estimate the sublimation pressure of solids. ii) the genetic algorithms method has shown to be a good tool to solve the optimization problem studied here, providing accurate global optima. Acknowledgements
The authors thanks the support of the National Commission for Scientific and Technological Research (CONICYT-Chile), through the research grants FONDECYT 1050410 and 1040285. JOV also thanks the Direction of Research of the University of La Serena-Chile for permanent support through several research grants and the Center for Technological Information (CIT, La Serena-Chile), for computer and library support. CAF thank the Dept. of Physics of the University of Concepción-Chile for special support that made possible the preparation of this work.
References
[1] J.M. Prausnitz, R.N. Lichtenthaler, E. Gomes de Azevedo, Molecular Thermodynamics of Fluid-Phase Equilibria. Prentice Hall International Series, New Jersey, USA, (1999).
[2] S.M. Walas, Phase Equilibria in Chemical Engineering, Butterworth Pub.-USA, (1985).
[3] D.Y. Peng, D.B. Robinson, Ind. Eng. Chem. Fundam., 15, 59-64 (1976).
[4] D.S. Wong, S.I. Sandler, AIChE Journal 38 671-680 (1992).
[5] K.P. Johnston, D.H. Ziger, C.A. Eckert, Ind. Eng. Chem. Fundam. 21, 191-197 (1982).
[6] G. Anitescu, L.L Tavlarides, J. Sup. Fluids 10, 175-189 (1997).
[7] W. J. Schmitt, R.C. Reid, Fluid Phase Equilib. 32, 77-99 (1986).
[8] M. McHugh, M.E. Paulaitis, J.Chem.Eng. Data, 25 326-329 (1980). <>[9] J.O. Valderrama, J. Zavaleta, Ind. Eng. Chem. Res., 44, 4824-4833 (2005).