Liquid density of HFE-7000 and HFE-7100 from T = (283 to 363) K at pressures up to 100 MPa
Graphical abstract
Compressed density data of HFE-7000 (a) and HFE-7100 (b).
Introduction
During the last decade, intensive efforts have been devoted to identify replacements to the traditional fluoro-chems compounds which have been proven to deplete the ozone layer and enhance greenhouse effect. Hydrofluoroether fluids (HFEs) are being proposed as environmentally friendly alternatives to other halogenated compounds because of their nearly zero ozone depletion, relatively low global warming potential, short atmospheric lifetimes and low toxicity [1], [2]. They have been used in various industrial applications as refrigerants, cleaning solvents of electronic components, foaming agent, heat transfer fluids and so on [3].
In spite of the widespread application of HFEs, there is still much to learn about their thermophysical properties. For HFE-7000 and HFE-7100, very limited experimental data has been published. Table 1 gives an overview of the literature which presents the liquid density data for HFE-7000 and HFE-7100. The corresponding temperature and pressure region and the number of data points are also provided.
For HFE-7000, Ohta et al. [4] presented the saturated-liquid and compressed-liquid densities from T = (250 to 370) K and pressures up to 3 MPa. Klomfar [7] investigated the compressed liquid density in the temperature range of (209 to 353) K and pressures up to 40 MPa. Additionally, references [1], [5], [6] reported the liquid density of HFE-7000 at normal temperatures and pressures. For HFE-7100, Pineiro et al. [9] measured the liquid density between T = (283.15 and 313.15) K at pressures up to 40 MPa. Minamihounoki et al. [8], [10], [11] only reported the density of HFE-7100 in the normal pressures and temperatures. Shiflett et al. [12] presented the liquid density data as a linear equation which was valid in the temperature range of (283 to 333) K and pressures at 0.1 MPa.
In previous work, our group has conducted compressed-liquid densities of HFE-7200 (1-Ethoxy-1,1,2,2,3,3,4,4,4-nonafluorobutane) and HFE-7500 (3-ethoxyperfluoro(2-methylhexane)) in a wide range of temperatures and pressure [13]. As a continuous research, in this work, measurements of compressed-liquid densities were carried out for HFE-7000 and HFE-7100 over the temperature range from (283 to 363) K with pressures up to 100 MPa using a vibrating-tube densimeter system. The experimental data were correlated to a modified Tait equation, with which the isothermal compressibility and isobaric thermal expansivity have also been calculated.
Section snippets
Samples
HFE-7000 and HFE-7100 were supplied by the 3M Company (mass purity > 0.995). HFE-7100 consists of two inseparable isomers (nonafluoro-iso-butylmethyether and nonafluoro-n-butylmethylether) with essentially identical properties. These isomers are considered to be azeotrope and azeotropic mixtures are equivalently handled with pure substance. In this work, HFE-7100 was used as the sample supplied without out any separation of the isomers. The water contents of HFE-7000 and HFE-7100 were tested with
Density
The compressed liquid densities of HFE-7000 and HFE-7100 were measured between T = (283 to 363) K with pressures up to 100 MPa. As the vibrating tube could be only used to measure the liquid density, the vapor pressure of HFE-7000 and HFE-7100 were estimated with equations in reference [12] to select the initial pressure along each isotherms. A total of 138 and 141 data points are reported for HFE-7000 and HFE-7100, separately. The uncertainties of each experimental data point were calculated with
Conclusion
In present work, a total of 279 compressed liquid densities of HFE-7000 and HFE-7100 along nine isotherms between T = (283 and 363) K with pressures up to 100 MPa were presented. The maximum expanded uncertainty with a level of confidence of 0.95 (k = 2) of HFE-7000 and HFE-7100 are 0.04% and 0.03%, respectively. The experimental data were fitted with a modified Tait equation with low standard deviations. And the isobaric thermal expansivity, αp, and the isothermal compressibility, κT, were derived
Acknowledgment
The authors acknowledge the financial support of the Specialized Research Fund for the Doctoral Program of Higher Education of China (No. 20100201120014), Natural Science Foundation of Jiangsu Province, China (No. SBK201122327) and Natural Science Foundation of Changchun Normal University (Grant 2014).
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