(202f) Investigating the Ability of the RK-Aspen Equation of State to Correlate the High-Pressure Phase Behavior of Binary and Ternary CO2-Containing Systems
AIChE Annual Meeting
2024
2024 AIChE Annual Meeting
Engineering Sciences and Fundamentals
High Pressure Phase Equilibria and Modeling
Monday, October 28, 2024 - 5:10pm to 5:30pm
Many studies have looked at the phase behavior and thermodynamic modelling of CO2-containing systems [4-15] and have shown that mixtures of CO2 + 1-alcohols + n-alkanes [7-14], CO2 + n-carboxylic acids + n-alkanes and CO2 + methyl ester + n-alkanes [8,15] display complex phase behavior phenomenon such as co-solvency. This complicates the thermodynamic modelling of these systems.
Studies by Fourie [16], Ferreira [17] and Latsky [18] investigated the thermodynamic modelling of CO2 + 1-alcohol + nÂâalkane systems. Fourie [16] and Ferreira [17] considered the ability of either Soave-Redlich Kwong (SRK) type cubic equations of state or the PC-SAFT [19,20] model to correlate the phase behavior and found that the cubic equations of state outperformed the PC-SAFT model. Ferreira [17] and Latsky [18] further considered the effect that the type of source data used to regress parameters have on model performance for the SRK type models. Ferreira [17] considered the effect of regressing solute + solute binary interaction parameters (BIPs) for the RK-Aspen [21], PSRK [22] and SR-Polar [21] models using low-pressure vapour liquid equilibrium (LPVLE), high-pressure bubble- and dew-point (HPBDP) and high-pressure vapor liquid equilibrium data (HPVLE) for the CO2 + 1-decanol + n-tetradecane system. Latsky [18] further evaluated the effect of utilising HPBDP versus HPVLE data to regress parameters for the SRK [23], RK-Aspen, PSRK and CPA [24] models for the quarternary and comprising ternary systems of CO2 + 1-decanol + n-dodecane + 3,7-dimethyl-1-octanol.
Ferreira [17] found that the RK-Aspen model including solute + solute BIPs that are regressed to HPBDP data outperforms regressions conducted using HPVLE or LPVLE data for each of the models considered, while the findings by Latsky [18] supported this finding when comparing the regressions obtained using HPBDP or HPVLE data. This was a desirable outcome, since HPBDP data are much easier, faster and cheaper to measure than HPVLE data. These conclusions are true for CO2 + 1-alcohol + n-alkane systems, but evaluations for CO2 systems with other solutes, such as n-carboxylic acids and methyl esters, have not been made. The aim of this work is therefore to evaluate the ability of the RKâAspen equation of state to model CO2 + solute + solute systems, where the solutes are 1-alcohols, nâÂalkanes, n-carboxylic acids and methyl esters. This aim will be achieved by:
- Investigating the ability of the RK-ASPEN model to predict the ternary phase behavior by only incorporating solvent (CO2) + solute BIPs regressed to binary data;
- Investigating the ability of the RK-ASPEN to correlate the ternary mixture data for several solute + solute combinations; and
- Investigating the effect of using either HPBDP or HPVLE data to regress the solute + solute BIPs on the model performance.
As the purpose of the study is to use the RK-Aspen model and to ultimately implement the model in a process simulator, Aspen Plus® V14 was used in combination with the Aspen Simulation Workbook (ASW) in MSExcel.
The RK-Aspen model is a modified version of the SRK equation of state where an additional pure component parameter, the polar parameter η, is introduced in the alpha function. The added parameter allows for improved correlation of the pure component phase behavior. The polar parameters were regressed against pure component vapor pressure data obtained from the NIST ThermoData Engine (TDE) available within Aspen Plus®, using the Aspen Plus® Data Regression System (DRS). The maximum likelihood objective function, minimising the pure component vapor pressure, was employed, with the Britt-Luecke minimisation algorithm.
The model is further extended to mixtures through incorporation of quadratic mixing rules and the inclusion of two BIPs. In this work the solvent + solute BIPs were regressed from previously measured binary solvent + solute phase behaviour data using the Aspen Plus® DRS through minimization of the maximum likelihood objective function together with the Britt-Luecke algorithm. For systems where only HPBDP data were available, the data were converted to HPVLE data by fitting pressure-composition curves through the HPBDP data and then calculating the compositions of the co-existing phases at 0.2 MPa intervals.
The method of correlation of the solute + solute BIPs depends on the type of source data used. For the LPVLE and HPVLE data, where the compositions of the co-existing phases are known, the same method as for the solvent + solute BIPs is used. For the HPBDP data an alternative method is required as the data are phase boundary data and therefore compositions of the co-existing phases are not known. Here the bubble or dew point is pressure predicted at a set temperature and composition using a flash drum in Aspen Plus® and the BIPs are systematically varied to minimize the error in the pressure prediction. The ASW in MSExcel was used to allow for a fine grid in the minimization procedure.
The results have shown where the inclusion of the solute + solute BIPs are required and in which types of systems HPVLE data are required for correlation of the solute + solute BIPs versus where only HPBDP data are needed. The study has also shown how the molecular interactions such as association and hydrogen bonding differs in different types of systems and how well the RK-Aspen model can predict or correlate the various interactions.
Although the RK-Aspen model has been shown to outperform other models such as CPA or PC-SAFT for CO2 + 1-alcohol + n-alkane systems [16-18], it would be prudent to further investigate if these results can be generalised to systems containing other functional groups such as n-carboxylic acids and/or methyl esters.
References
[1] G.J.K. Bonthuys, C.E. Schwarz, A.J. Burger, J.H. Knoetze, J. Supercrit. Fluids. 57 (2011) 101â111.
[2] C.E. Schwarz, G.J.K. Bonthuys, R.F. van Schalkwyk, D.L. Laubscher, A.J. Burger, J.H. Knoetze, J. Supercrit. Fluids. 58 (2011) 352â359.
[3] W. Eisenbach, Ber. Bunsenges. Phys. Chem., 88 (1984) 882-887.
[4] R. Dohrn, S. Peper, J.M.S. Fonseca, Fluid Phase Equilib. 288 (2010) 1â54.
[5] S. Peper, J.M.S. Fonseca, R. Dohrn, Fluid Phase Equilib. 484 (2019) 126â 224.
[6] R. Dohrn, S. Peper, C. Secuianu, J.M.S. Fonseca, Fluid Phase Equilib. 579 (2024) 113978.
[7] K. Gauter, C.J. Peters, A.L. Scheidgen, G.M. Schneider, Fluid Phase Equilib. 171 (2000) 127-149.
[8] A.L. Scheidgen, G.M. Schneider, Fluid Phase Equilib. 194â197(2002) 1009-1028.
[9] A. Kordikowski, G.M. Schneider, Fluid Phase Equilib. 90 (1993) 149-162.
[10] M. Spee, G.M. Schneider, Fluid Phase Equilib. 65 (1991) 263-214.
[11] C. Latsky, C.E. Schwarz, Fluid Phase Equilib. 488 (2019) 87-98.
[12] C. Latsky, N.S. Mabena, C.E. Schwarz, J. Supercrit. Fluids. 149 (2019) 138-150.
[13] C. Latsky, B. Cordeiro, C.E. Schwarz, Fluid Phase Equilib. 521 (2020) 112702.
[14] C. Secuianu, V. Feroiu, D. Geana, Fluid Phase Equilib. 261 (2007) 337â342.
[15] S.H. Du Plessis, C.E. Schwarz, J. Chem. Eng. Data Article ASAP, DOI: 10.1021/acs.jced.3c00725
[16] F.C. van N. Fourie, Doctoral Dissertation in Chemical Engineering, Stellenbosch University, 2018
[17] M. Ferreira, Doctoral Dissertation in Chemical Engineering, Stellenbosch University, 2018
[18] C. Latsky, Doctoral Dissertation in Chemical Engineering, Stellenbosch University, 2019
[19] J. Gross, G. Sadowski, Ind. Eng. Chem. Res. 40 (2001) 1244-1260.
[20] J. Gross, G. Sadowski, Ind. Eng. Chem. Res. 41 (2002) 5510-5515.
[21] Aspen Technology Inc., Aspen Plus V14, 2024.
[22] T. Holderbaum and J. Gmehling, Fluid Phase Equilibria 70 (1991) 251-265.
[23] G. Soave, Chemical Engineering Science 27 (1972) 1197-1203.
[24] G. M. Kontogeorgis, E. C. Voutsas, I. V. Yakoumis and D. P. Tassios, Industrial and Engineering Chemistry Research 35 (1996) 4310-4318.