Isothermal phase (vapour + liquid) equilibrium data for binary mixtures of propene (R1270) with either 1,1,2,3,3,3-hexafluoro-1-propene (R1216) or 2,2,3-trifluoro-3-(trifluoromethyl)oxirane in the temperature range of (279 to 318) K
Graphical abstract
Introduction
This study is part of an on-going research programme investigating the thermodynamic properties of fluorocarbons and their mixtures [1], [2], [3], [4], [5], [6], and more specifically isothermal phase behaviour for binary mixtures involving either 1,1,2,3,3,3-hexafluoro-1-propene or 2,2,3-trifluoro-3-(trifluoromethyl)oxirane [6], [7], [8], [9], [10], [11], [12]. (Vapour + liquid) equilibrium (VLE) data play an integral part in the design process of numerous unit operations and chemical processes. Furthermore, VLE data is a core necessity for the development and validation of correlative and predictive thermodynamic models. Accordingly, accurate VLE data are required for the calculation of interaction energies between functional groups for group contribution methods such as PSRK [13].
VLE data were measured for the binary systems of propene (R1270) + 1,1,2,3,3,3-hexafluoro-1-propene (R1216), and R1270 + trifluoro-3-(trifluoromethyl)oxirane. Trifluoro-3-(trifluoromethyl)oxirane is more commonly known as hexafluoropropylene oxide (HFPO). To the best of our knowledge no VLE data have been published for the R1270 + HFPO binary system, and thus, all data presented herein for this system are new data. Concerning the R1270 + R1216 binary system, isothermal VLE data have been measured by Coquelet et al. [6] in the temperature range from (263.17 to 353.14) K. The data corresponding to this work were measured within the same temperature range, but at different isothermal conditions. Consequently, they may be considered as useful complementary data. These two binary systems exhibit homogenous pressure-maximum (positive) azeotropes within the investigated temperature range. The new experimental data were correlated with the Peng–Robinson (PR) [14] equation of state (EoS) integrating the Mathias–Copeman (MC) alpha function [15], the Wong–Sandler (WS) mixing rule [16] and the Non-Random Two Liquid (NRTL) activity coefficient model [17].
Section snippets
Materials
Propene was supplied by Air Products (South Africa) with a certified purity greater than 0.9995 in volume fraction. 1,1,2,3,3,3-Hexafluoro-1-propene and 2,2,3-trifluoro-3-(trifluoromethyl)oxirane were supplied by Pelchem (South Africa) with a certified purity greater than 0.999 in volume fraction. Apart from degassing via periodic vapour withdrawal, no further purification was undertaken. Gas chromatographic (GC) analysis is a classical method to validate the purities of each component.
Results and discussion
Experimental vapour pressure data for R1270 are reported in table 3. The P–T data were modelled using the PR equation of state with the MC alpha function. The deviations of the data correlated by the model from experimental data are listed in table 3. The model accurately represents the vapour pressure data for R1270. The experimental vapour pressure data for R1270 were also compared to reference values from REFPROP [25], the resulting average absolute deviation for pressure is 0.33%.
P–x–y data
Conclusion
P-x-y data are reported for binary mixtures of propene with either 1,1,2,3,3,3-hexafluoro-1-propene or 2,2,3-trifluoro-3-(trifluoromethyl)oxirane at temperatures ranging from (279.36 to 318.09) K. The two binary systems exhibit a pressure-maximum azeotrope at all measured temperatures. The data are well correlated using a single set of binary interaction parameters across the entire temperature range for each system using the Peng–Robinson equation of state including the Mathias–Copeman alpha
Acknowledgements
This work is based upon research supported by the National Research Foundation of South Africa under the South African Research Chair Initiative of the Department of Science and Technology.
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2018, International Journal of RefrigerationCitation Excerpt :Therefore, it is necessary to know fluid-phase behavior of such mixtures (Qian et al., 2017). In the literature, several different thermodynamic methods for modeling the experimental VLE data of perfluorocarbon-containing binary systems using cubic equations of state were proposed such as the PR EoS, the PR EoS with the Wong–Sandler (WS) mixing rule, the SRK EoS with the Wong–Sandler (WS) mixing rule, the PR EoS with the Huron–Vidal first-order (MHV1) mixing rule (Bengesai et al., 2016; Coquelet et al., 2010a; El Ahmar et al., 2011; Nelson et al., 2015, 2016a, 2016b; Subramoney et al., 2010, 2012, 2013a, 2013b, 2013c, 2015a, 2015b, 2015c; Tebbal et al., 2016; Tshibangu et al., 2013; Valtz et al., 2011) and the E-PPR78 model (Qian et al., 2017). Also, the Mathias–Copeman alpha function was used in the PR EoS and the non-random two liquid (NRTL) excess Gibbs energy model was proposed for the WS mixing rule.
Phase equilibrium and critical point data for ethylene and chlorodifluoromethane binary mixtures using a new “static-analytic” apparatus
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