| Literature DB >> 31384637 |
Abstract
In this Data in Brief article, we present predictive data for the vapor-liquid equilibria of the binary mixtures of HFO-1123 with R-32, HFO-1234yf, HFO-1234ze(E), R-134a and CO2 from molecular simulation. The VLE in the binary mixtures are then modeled by the PCP-SAFT equation of state. Therefore we determined PCP-SAFT parameters for the pure HFO compounds as well as binary interaction parameters for all mixtures. The simulation data and the PCP-SAFT modelling are discussed in a related research article (Raabe, 2019).Entities:
Keywords: HFO-1123; Molecular simulation; PCP-SAFT; Refrigerants; VLE
Year: 2019 PMID: 31384637 PMCID: PMC6661389 DOI: 10.1016/j.dib.2019.104014
Source DB: PubMed Journal: Data Brief ISSN: 2352-3409
Data from GEMC simulations for the VLE in binary mixtures of HFO-1123 with R-32, R-1234yf, R-1234ze(E) and R-134a: mole fraction in the saturated liquid (x) and vapor phase (y), and saturated densities ρL and ρV. Values in parentheses denote standard deviations.
| T (K) | p(MPa) | x1123 (mol mol−1) | y1123 (mol mol−1) | ρL (kg m−3) | ρV (kg m−3) |
|---|---|---|---|---|---|
| HFO-1123 + R-32 | |||||
| 220.0 | 0.10 | 0.082 (0.003) | 0.167 (0.013) | 1254.0 (3.2) | 3.3 (0.1) |
| 0.11 | 0.216 (0.014) | 0.351 (0.006) | 1270.0 (1.6) | 3.9 (0.1) | |
| 0.12 | 0.361 (0.013) | 0.500 (0.011) | 1283.5 (1.5) | 4.6 (0.1) | |
| 0.13 | 0.593 (0.002) | 0.671 (0.003) | 1304.7 (1.0) | 5.3 (0.1) | |
| 230.0 | 0.17 | 0.134 (0.009) | 0.235 (0.012) | 1229.2 (1.1) | 5.5 (0.1) |
| 0.18 | 0.216 (0.013) | 0.338 (0.014) | 1238.5 (1.4) | 6.2 (0.1) | |
| 0.19 | 0.321 (0.009) | 0.446 (0.009) | 1248.5 (1.3) | 6.9 (0.1) | |
| 0.20 | 0.414 (0.008) | 0.530 (0.005) | 1258.0 (2.8) | 7.5 (0.1) | |
| 0.21 | 0.594 (0.008) | 0.645 (0.014) | 1260.4 (9.2) | 8.1 (0.2) | |
| 270.0 | 0.80 | 0.117 (0.004) | 0.174 (0.006) | 1087.8 (0.7) | 24.3 (0.1) |
| 0.85 | 0.242 (0.008) | 0.319 (0.008) | 1098.5 (1.4) | 27.7 (0.1) | |
| 0.90 | 0.385 (0.004) | 0.456 (0.004) | 1110.3 (1.2) | 31.3 (0.1) | |
| 290.0 | 1.45 | 0.116 (0.001) | 0.157 (0.002) | 998.7 (2.2) | 44.5 (0.2) |
| 1.50 | 0.173 (0.001) | 0.225 (0.002) | 1005.9 (1.9) | 47.7 (0.3) | |
| 1.55 | 0.268 (0.002) | 0.324 (0.001) | 1010.3 (0.5) | 51.7 (0.1) | |
| 1.60 | 0.350 (0.005) | 0.404 (0.004) | 1016.9 (1.6) | 55.6 (0.3) | |
| HFO-1123 + R-1234yf | |||||
| 220.0 | 0.05 | 0.201 (0.008) | 0.558 (0.012) | 1339.4 (3.1) | 2.7 (0.1) |
| 0.075 | 0.443 (0.016) | 0.800 (0.012) | 1335.6 (2.3) | 3.7 (0.1) | |
| 0.1 | 0.657 (0.024) | 0.905 (0.008) | 1334.0 (2.7) | 4.8 (0.1) | |
| 240.0 | 0.15 | 0.302 (0.015) | 0.638 (0.019) | 1277.0 (2.5) | 7.4 (0.1) |
| 0.2 | 0.459 (0.012) | 0.771 (0.013) | 1275.8 (3.0) | 9.5 (0.1) | |
| 0.3 | 0.863 (0.009) | 0.960 (0.003) | 1266.6 (2.2) | 13.5 (0.1) | |
| 270.0 | 0.4 | 0.183 (0.016) | 0.402 (0.025) | 1185.3 (2.6) | 20.0 (0.2) |
| 0.5 | 0.319 (0.010) | 0.581 (0.011) | 1182.2 (1.3) | 23.8 (0.1) | |
| 0.65 | 0.554 (0.013) | 0.782 (0.009) | 1171.1 (2.0) | 29.4 0.1) | |
| 0.75 | 0.695 (0.006) | 0.866 (0.003) | 1165.4 (1.7) | 33.4 (0.1) | |
| 0.85 | 0.830 (0.010) | 0.932 (0.005) | 1158.1 (3.1) | 37.3 (0.1) | |
| 290.0 | 0.75 | 0.202 (0.009) | 0.396 (0.011) | 1111.2 (3.3) | 37.1 (0.2) |
| 1.0 | 0.408 (0.010) | 0.630 (0.011) | 1101.7 (2.1) | 47.0 (0.3) | |
| 1.25 | 0.628 (0.007) | 0.804 (0.005) | 1087.4 (2.5) | 56.6 (0.2) | |
| 1.5 | 0.836 (0.008) | 0.924 (0.004) | 1069.6 (2.9) | 67.2 (0.2) | |
| 310.0 | 1.1 | 0.087 (0.008) | 0.173 (0.002) | 1035.2 (1.9) | 59.0 (0.4) |
| 1.25 | 0.183 (0.009) | 0.326 (0.012) | 1030.0 (3.0) | 64.5 (0.4) | |
| 1.5 | 0.327 (0.010) | 0.508 (0.012) | 1020.2 (2.3) | 74.7 (0.4) | |
| 1.75 | 0.474 (0.015) | 0.652 (0.015) | 1004.7 (4.6) | 84.6 (1.0) | |
| 2.0 | 0.602 (0.008) | 0.755 (0.006) | 992.6 (2.5) | 95.9 (0.5) | |
| 2.25 | 0.747 (0.006) | 0.854 (0.004) | 969.8 (2.2) | 106.4 (0.7) | |
| HFO-1123 + R-1234ze(E) | |||||
| 250.0 | 0.2 | 0.318 (0.009) | 0.726 (0.007) | 1306.6 (2.0) | 9.2 (0.1) |
| 0.3 | 0.527 (0.008) | 0.863 (0.007) | 1288.5 (0.6) | 13.4 (0.1) | |
| 0.4 | 0.786 (0.022) | 0.952 (0.007) | 1257.8 (4.7) | 17.5 (0.1) | |
| 270.0 | 0.3 | 0.148 (0.005) | 0.435 (0.013) | 1260.1 (1.9) | 14.4 (0.1) |
| 0.4 | 0.282 (0.007) | 0.631 (0.012) | 1249.2 (1.5) | 18.2 (0.1) | |
| 0.6 | 0.550 (0.020) | 0.839 (0.011) | 1217.3 (4.4) | 26.0 (0.1) | |
| 0.8 | 0.802 (0.017) | 0.942 (0.006) | 1182.8 (5.4) | 34.8 (0.3) | |
| 290.0 | 0.6 | 0.172 (0.005) | 0.420 (0.005) | 1193.4 (2.8) | 28.3 (0.1) |
| 0.8 | 0.355 (0.006) | 0.653 (0.010) | 1167.2 (1.6) | 35.6 (0.2) | |
| 1.0 | 0.486 (0.016) | 0.759 (0.010) | 1153.3 (6.1) | 44.1 (0.3) | |
| 1.2 | 0.643 (0.014) | 0.853 (0.010) | 1128.4 (4.3) | 52.5 (0.1) | |
| 1.4 | 0.791 (0.007) | 0.921 (0.003) | 1101.5 (3.4) | 61.5 (0.1) | |
| 310.0 | 0.8 | 0.049 (0.004) | 0.131 (0.007) | 1129.4 (3.2) | 40.3 (0.2) |
| 1.0 | 0.157 (0.006) | 0.346 (0.013) | 1117.1 (2.5) | 47.9 (0.2) | |
| 1.2 | 0.266 (0.013) | 0.500 (0.019) | 1101.0 (5.6) | 55.9 (0.5) | |
| 1.6 | 0.458 (0.005) | 0.690 (0.007) | 1074.1 (1.8) | 73.4 (0.7) | |
| 2.0 | 0.652 (0.012) | 0.824 (0.007) | 1036.1 (4.5) | 91.6 (0.3) | |
| 2.4 | 0.832 (0.008) | 0.922 (0.004) | 989.7 (4.3) | 112.3 (0.5) | |
| HFO-1123 + R-134a | |||||
| 250.0 | 0.2 | 0.203 (0.014) | 0.485 (0.022) | 1335.3 (2.8) | 9.4 (0.1) |
| 0.3 | 0.476 (0.017) | 0.763 (0.011) | 1303.0 (3.4) | 13.4 (0.1) | |
| 0.4 | 0.728 (0.017) | 0.901 (0.010) | 1270.1 (3.4) | 17.7 (0.1) | |
| 270.0 | 0.4 | 0.172 (0.010) | 0.389 (0.018) | 1274.7 (2.3) | 18.4 (0.1) |
| 0.5 | 0.337 (0.008) | 0.603 (0.011) | 1252.7 (1.8) | 22.2 (0.1) | |
| 0.6 | 0.489 (0.008) | 0.737 (0.005) | 1230.6 (1.8) | 26.2 (0.1) | |
| 0.7 | 0.608 (0.017) | 0.817 (0.010) | 1215.1 (4.9) | 30.5 (0.1) | |
| 0.825 | 0.780 (0.014) | 0.908 (0.006) | 1188.7 (3.6) | 36.0 (0.1) | |
| 290.0 | 0.8 | 0.206 (0.006) | 0.399 (0.003) | 1199.1 (0.7) | 36.4 (0.1) |
| 1.0 | 0.400 (0.012) | 0.624 (0.012) | 1169.4 (3.3) | 44.3 (0.2) | |
| 1.2 | 0.565 (0.013) | 0.758 (0.009) | 1142.0 (4.9) | 52.8 (0.3) | |
| 1.4 | 0.752 (0.018) | 0.880 (0.019) | 1109.0 (4.4) | 61.7 (0.2) | |
| 310.0 | 1.2 | 0.126 (0.007) | 0.243 (0.013) | 1128.3 (1.5) | 56.1 (0.1) |
| 1.4 | 0.232 (0.006) | 0.396 (0.010) | 1112.6 (2.5) | 64.6 (0.4) | |
| 2.2 | 0.694 (0.011) | 0.816 (0.008) | 1019.2 (4.4) | 101.9 (0.5) | |
| 2.4 | 0.794 (0.006) | 0.880 (0.004) | 994.9 (2.8) | 111.8 (0.2) | |
Data from GEMC simulations for the VLE in binary mixture CO2 + HFO-1123: mole fraction in the saturated liquid (x) and vapor phase (y), and saturated densities ρL and ρV. Values in parentheses denote standard deviations.
| T (K) | p(MPa) | xCO2 (mol mol−1) | yCO2 (mol mol−1) | ρL (kg m−3) | ρV (kg m−3) |
|---|---|---|---|---|---|
| CO2 + HFO-1123 | |||||
| 250.0 | 1.0 | 0.382 (0.005) | 0.654 (0.006) | 1171.2 (2.2) | 30.6 (0.5) |
| 1.5 | 0.811 (0.011) | 0.921 (0.006) | 1087.4 (3.6) | 40.0 (0.2) | |
| 270.0 | 1.5 | 0.252 (0.006) | 0.467 (0.010) | 1109.7 (2.6) | 51.8 (0.6) |
| 2.0 | 0.475 (0.005) | 0.692 (0.006) | 1069.4 (3.2) | 61.1 (0.7) | |
| 2.2 | 0.570 (0.007) | 0.763 (0.006) | 1051.0 (2.4) | 65.1 (0.7) | |
| 2.5 | 0.700 (0.004) | 0.845 (0.004) | 1022.7 (3.4) | 70.6 (1.3) | |
| 2.7 | 0.794 (0.007) | 0.897 (0.005) | 1001.8 (3.4) | 74.5 (1.0) | |
| 290.0 | 2.5 | 0.237 (0.005) | 0.401 (0.008) | 1015.9 (4.6) | 93.3 (1.5) |
| 3.0 | 0.378 (0.003) | 0.561 (0.006) | 984.7 (4.8) | 102.0 (2.6) | |
| 3.5 | 0.520 (0.005) | 0.683 (0.005) | 958.0 (3.5) | 115.3 (1.3) | |
| 4.0 | 0.651 (0.005) | 0.783 (0.004) | 923.6 (4.1) | 125.2 (2.2) | |
| 4.5 | 0.784 (0.007) | 0.870 (0.005) | 889.3 (6.0) | 137.4 (3.5) | |
Fig. 1Correlation of the VLCC and vapor pressure curve of R-1234ze(E)=▲, R-1234yf=● and HFO-1123=■by the PCP-SAFT (red line) and available EOS models in REFPROP [8](dark grey line). Shown as filled symbols are experimental VLE data for R-1234ze(E) ([7], [9], [10], [11]), R-1234yf ([12]) and HFO-1123 ([13], [14]). Also given are GEMC simulation results ⊠ for HFO-1123 that were employed in the fitting (∃, [5]).
PCP-SAFT parameters for the refrigerants studied in this work.
| Refrigerant | μ* | Q | Source | ||||
|---|---|---|---|---|---|---|---|
| HFO-1123 | 82.02 | 1.9620 | 3.45868 | 172.948 | 5.348 | this work | |
| R-32 | 52.02 | 2.47192 | 2.79714 | 161.6614 | 1.978 | Vinš et al. | |
| R-134a | 102.03 | 3.14704 | 3.04554 | 165.3555 | 2.058 | Vinš et al. | |
| R-1234yf | 114.04 | 1.63761 | 4.23860 | 185.2610 | 0.9887 | 10.35 | this work |
| R-1234ze(E) | 114.04 | 1.97291 | 3.918 | 188.7388 | 8.98 | this work | |
| CO2 | 44.01 | 1.5131 | 3.1869 | 163.33 | 4.4 | Gross |
PCP-SAFT Interaction parameters k, and resulting deviation from the GEMC simulation.
| Refrigerant mixture | Δ | Δ | Δ | Δ | |
|---|---|---|---|---|---|
| HFO-1123 + R-32 | 0.0358 | 1.5 | 0.0209 | 1.3 | 5.6 |
| HFO-1123 + R-1234ze(E) | 0.0048 | 1.6 | 0.0053 | 2.2 | 1.7 |
| HFO-1123 + R-1234yf | −0.0083 | 2.6 | 0.0084 | 1.0 | 3.4 |
| HFO-1123 + R-134a | −0.0003 | 1.2 | 0.0033 | 0.6 | 1.9 |
| CO2 + HFO-1123 | 0.0030 | 1.2 | 0.0039 | 1.7 | 3.3 |
Specifications Table
| Subject area | Chemistry, chemical engineering |
|---|---|
| More specific subject area | Molecular simulation, thermophysical properties |
| Type of data | Tables, figure |
| How data was acquired | The VLE data was acquired by Gibbs Ensemble Monte Carlo (GEMC) simulation using the code TOWHEE |
| Data format | Filtered, analyzed. |
| Experimental factors | Simulations were performed in NPT ensemble. Each system consisted of 432 molecules. For each data point, the simulation was equilibrated for 200,000 cycles. The production runs consisted of 300,000–500.000 cycles. Standard deviations of all ensemble averages were calculated by the standard block averaging technique. |
| Experimental features | GEMC molecular simulation results for the compositions and saturated densities of the VLE in the binary mixtures for imposed temperatures and pressures. The data are in the temperature range T = (220–310) K |
| Data source location | Braunschweig, Germany, TU Braunschweig, Institut für Thermodynamik |
| Data accessibility | data is with this article |
| Related research article | Molecular Simulation Studies on Refrigerants. Past – Present – Future. |
This article provides first data for the VLE properties of binary mixtures of HFO-1123 with R-32, R-1234yf, R-1234ze(E), R-134a and CO2, which are discussed as new refrigerants blends The new PCP-SAFT parameters (EOS parameters ε, σ, μ and Q) provided in this article allow for an accurate modelling of the pure compounds HFO-1123, -1234yf,-1234ze(E) The kij interaction parameters in this article allow for a computation of the VLE properties of binary mixtures of HFO-1123 with R-1234yf, R-1234ze(E), R-32, R-134a, CO2 by the PCP-SAFT equation of state The data and modelling approach provided in this article may be used by researchers in the field of refrigeration to evaluate the performance of new HFO-1123 based refrigerant blends |