对氢经济具有重要意义的 ($H_{2}$ + $C_{3}H_{8}$)系统的热力学特性分析:实验($p$、$ρ$、$T$)测定和状态方程建模

Daniel Lozano-Martín, Peyman Khanipour, Heinrich Kipphardt, Dirk Tuma, César R. Chamorro
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摘要

为了将氢气逐步引入能源市场,研究氢气与天然气(NG)和液化石油气(LPG)典型成分的混合物的性质具有重要意义。这项工作旨在为三种氢-丙烷混合物提供精确的实验($p$, $\rho$, $T$)数据,这些混合物的标称成分(物质的量,mol/mol)为 (0.95$H_{2}$+0.05$C_{3}H_{8}$)、(0.90$H_{2}$+0.10$C_{3}H_{8}$)和(0.83$H_{2}$+0.17$C_{3}H_{8}$)三种氢丙烷混合物在 250、275、300、325、350 和 375 K 温度和 20 MPa 压力下的数据。使用单沉式密度计测定混合物的密度。实验密度数据与两个参考状态方程(GERG-2008 和 AGA8-DC92)计算得出的密度进行了比较。与 GERG-2008 EoS 的相对偏差系统地大于与 AGA8-DC92 的相对偏差。丙烷含量为 5%的混合物的偏差在 0.5%范围内,但丙烷含量为 10%和 17%的混合物的偏差高于 0.5%,尤其是在低温高压条件下。最后,应用两种不同的统计状态方程对新的实验数据集进行了处理:通过第二和第三维里亚尔系数($B$($T$, $x$)和$C$($T$, $x$))的维里亚尔状态方程,以及 PC-SAFT 状态方程。
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Thermodynamic characterization of the ($H_{2}$ + $C_{3}H_{8}$) system significant for the hydrogen economy: Experimental ($p$, $ρ$, $T$) determination and equation-of-state modelling
For the gradual introduction of hydrogen in the energy market, the study of the properties of mixtures of hydrogen with typical components of natural gas (NG) and liquefied petroleum gas (LPG) is of great importance. This work aims to provide accurate experimental ($p$, $\rho$, $T$) data for three hydrogen-propane mixtures with nominal compositions (amount of substance, mol/mol) of (0.95$H_{2}$ + 0.05$C_{3}H_{8}$), (0.90$H_{2}$ + 0.10$C_{3}H_{8}$), and (0.83$H_{2}$ + 0.17$C_{3}H_{8}$), at temperatures of 250, 275, 300, 325, 350, and 375 K, and pressures up to 20 MPa. A single-sinker densimeter was used to determine the density of the mixtures. Experimental density data were compared to the densities calculated from two reference equations of state: the GERG-2008 and the AGA8-DC92. Relative deviations from the GERG-2008 EoS are systematically larger than those from the AGA8-DC92. They are within the $\pm$0.5% band for the mixture with 5% of propane, but deviations are higher than 0.5% for the mixtures with 10% and 17% of propane, especially at low temperatures and high pressures. Finally, the sets of new experimental data have been processed by the application of two different statistical equations of state: the virial equation of state, through the second and third virial coefficients, $B$($T$, $x$) and $C$($T$, $x$), and the PC-SAFT equation of state.
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