The precise measurement of the (vapour + liquid) equilibrium properties for (CO2 + isobutane) binary mixtures☆
Introduction
Natural refrigerant mixtures with CO2 as the main component are expected to be one of the most promising long-term alternative fluids for refrigeration and heat-pump systems. For successful developments in this area, new reliable thermodynamic property models with high accuracy are required for these mixtures. In addition, a database of various thermophysical properties for mixtures over a wide range of temperatures and pressures is needed for the generalisation of Helmholtz-type equations of state (EOS). These requirements dictate that several researchers conduct a number of these measurements in the near future. Recently, several sets of reliable data for natural refrigerant mixtures have been published by Prof. Uematsu’s group for PρTx [1], [2], [3], [4], saturation properties [5], and critical parameters [6]. Literature data have also been published relatively recently for the (CO2 + propane) mixture [7], [8].
In this study, we attempted to measure the (vapour + liquid) equilibrium (VLE) properties, including bubble point pressures (Pbub) and dew point pressures (Pdew), for (CO2 + hydrocarbon) mixtures with a wide range of compositions (CO2 mole fraction x = 0 to x = 1). A new re-circulation type of apparatus, which is one of the most reliable methods available for VLE studies, was used for these measurements. Several sets of calibration measurements were conducted, followed by measurements for (CO2 + propane). The data were systematically compared with literature data and the values predicted by the Peng–Robinson (PR) equation of state (EOS) with the newest binary interaction parameter [8]. This confirmed that the measurement method had sufficient reliability. Additionally, VLE data were also determined for (CO2 + isobutane) binary mixtures and compared with REFPROP ver.8.0 [9].
Section snippets
Experimental
The recirculation type apparatus (figure 1) included an optical cell with four windows and was immersed in a liquid bath. A platinum resistance thermometer was inserted directly into the cell and the temperature of the sample was measured within ±0.26 K. The pressure was measured with a pressure gauge within ±0.43%. The overall uncertainties (95% confidence level) in temperature and pressure measurements were estimated as 0.56 K and 0.86%, respectively.
The sample in the cell was circulated by two
Results and discussion
For this method, reduction of fluctuation and establishment of high repeatability are the most important elements for precise and reliable measurements. After obtaining more than 100 points of unacceptable data, we established an appropriate measurement procedure with high repeatability. To confirm the overall reliability and repeatability, we then performed measurements for the CO2/propane binary mixture.
As discussed in Section 1, this binary system is especially important due to the potential
Conclusions
We aimed to provide VLE data with more reliable behaviour for (CO2 + isobutane) binary mixtures. After calibration of the gas chromatograph and estimation of the expanded uncertainties, we performed measurements for the CO2/propane binary mixture. These results confirmed the reliability of the apparatus. Subsequent measurements for the (CO2 + isobutane) binary mixtures provided reliable results for the Pbub and Pdew in comparison to literature data published by Weber [15] in 1989.
In future, we will
Acknowledgements
This work was supported through 2008–2011 by the Grant-in-Aid for Scientific Research Fund (Project No. 20686016) by the Ministry of Education, Culture, Sports, Science and Technology, Japan.
We would like to thank Dr. K. Fujii, Dr. Y. Kayukawa, Prof. Y. Higashi, Dr. K. Tanaka, Prof. T. Tsuji, Prof. Y. Iwai, Prof. K. Fukuchi, and Mr. S. Aizawa for their kind advice and assistance, all of which were indispensable throughout the study.
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2021, Journal of Chemical ThermodynamicsCitation Excerpt :The average absolute relative deviations obtained for the xCO2≈0.6 (CO2 + C3H8) mixture are: 3.91% for data from [56], 2.77% from [57], 4.63% from [58], 2.83% from [59], 1.53% from [60], 4.48% fomr [61], 1.67% from [62], 3.93% from [62], and 1.43% from [64]. Lower deviations (in general) were found for the xCO2≈0.8 (CO2 + C3H8) mixture: 3.78% from [56], 1.70% from [57], 2.27% from [58], 1.83% from [59], 1.38% from [60], 2.95% from [61], 2.09% from [62], 3.95% from [63], 1.21% from [64], and 4.72% from [65]. These values are mostly in agreement with the uncertainty of the EoS.
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2021, Journal of Chemical ThermodynamicsCitation Excerpt :Before introducing each sample into the apparatus, the materials were degassed at least three times by freeze–pump–thaw cycling with liquid nitrogen. The measurement apparatus is a recirculation-type device developed by Akico Co. Ltd. (Tokyo, Japan); the details of this apparatus have been described in prior publications [7,8]. A temperature-controlled optical cell of 380 cm3 inner volume was filled with a mixture sample in the two-phase state containing saturated liquid and saturated vapour.
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Presented at the 21st IUPAC International Conference on Chemical Thermodynamics held in Tsukuba Science City, Japan, 31 July to 06 August 2010.