Daniel Lozano-Martín, Peyman Khanipour, Heinrich Kipphardt, Dirk Tuma, César R. Chamorro
{"title":"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","authors":"Daniel Lozano-Martín, Peyman Khanipour, Heinrich Kipphardt, Dirk Tuma, César R. Chamorro","doi":"arxiv-2409.03647","DOIUrl":null,"url":null,"abstract":"For the gradual introduction of hydrogen in the energy market, the study of\nthe properties of mixtures of hydrogen with typical components of natural gas\n(NG) and liquefied petroleum gas (LPG) is of great importance. This work aims\nto provide accurate experimental ($p$, $\\rho$, $T$) data for three\nhydrogen-propane mixtures with nominal compositions (amount of substance,\nmol/mol) of (0.95$H_{2}$ + 0.05$C_{3}H_{8}$), (0.90$H_{2}$ + 0.10$C_{3}H_{8}$),\nand (0.83$H_{2}$ + 0.17$C_{3}H_{8}$), at temperatures of 250, 275, 300, 325,\n350, and 375 K, and pressures up to 20 MPa. A single-sinker densimeter was used\nto determine the density of the mixtures. Experimental density data were\ncompared to the densities calculated from two reference equations of state: the\nGERG-2008 and the AGA8-DC92. Relative deviations from the GERG-2008 EoS are\nsystematically larger than those from the AGA8-DC92. They are within the\n$\\pm$0.5% band for the mixture with 5% of propane, but deviations are higher\nthan 0.5% for the mixtures with 10% and 17% of propane, especially at low\ntemperatures and high pressures. Finally, the sets of new experimental data\nhave been processed by the application of two different statistical equations\nof state: the virial equation of state, through the second and third virial\ncoefficients, $B$($T$, $x$) and $C$($T$, $x$), and the PC-SAFT equation of\nstate.","PeriodicalId":501304,"journal":{"name":"arXiv - PHYS - Chemical Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"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\",\"authors\":\"Daniel Lozano-Martín, Peyman Khanipour, Heinrich Kipphardt, Dirk Tuma, César R. Chamorro\",\"doi\":\"arxiv-2409.03647\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For the gradual introduction of hydrogen in the energy market, the study of\\nthe properties of mixtures of hydrogen with typical components of natural gas\\n(NG) and liquefied petroleum gas (LPG) is of great importance. This work aims\\nto provide accurate experimental ($p$, $\\\\rho$, $T$) data for three\\nhydrogen-propane mixtures with nominal compositions (amount of substance,\\nmol/mol) of (0.95$H_{2}$ + 0.05$C_{3}H_{8}$), (0.90$H_{2}$ + 0.10$C_{3}H_{8}$),\\nand (0.83$H_{2}$ + 0.17$C_{3}H_{8}$), at temperatures of 250, 275, 300, 325,\\n350, and 375 K, and pressures up to 20 MPa. A single-sinker densimeter was used\\nto determine the density of the mixtures. Experimental density data were\\ncompared to the densities calculated from two reference equations of state: the\\nGERG-2008 and the AGA8-DC92. Relative deviations from the GERG-2008 EoS are\\nsystematically larger than those from the AGA8-DC92. They are within the\\n$\\\\pm$0.5% band for the mixture with 5% of propane, but deviations are higher\\nthan 0.5% for the mixtures with 10% and 17% of propane, especially at low\\ntemperatures and high pressures. Finally, the sets of new experimental data\\nhave been processed by the application of two different statistical equations\\nof state: the virial equation of state, through the second and third virial\\ncoefficients, $B$($T$, $x$) and $C$($T$, $x$), and the PC-SAFT equation of\\nstate.\",\"PeriodicalId\":501304,\"journal\":{\"name\":\"arXiv - PHYS - Chemical Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Chemical Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.03647\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Chemical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03647","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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.