Speed of sound data, derived perfect-gas heat capacities, and acoustic virial coefficients of a calibration standard natural gas mixture and a low-calorific $H_{2}$-enriched mixture
Daniel Lozano-Martín, David Vega-Maza, Alejandro Moreau, M. Carmen Martín, Dirk Tuma, José J. Segovia
{"title":"Speed of sound data, derived perfect-gas heat capacities, and acoustic virial coefficients of a calibration standard natural gas mixture and a low-calorific $H_{2}$-enriched mixture","authors":"Daniel Lozano-Martín, David Vega-Maza, Alejandro Moreau, M. Carmen Martín, Dirk Tuma, José J. Segovia","doi":"arxiv-2409.04094","DOIUrl":null,"url":null,"abstract":"This work aims to address the technical aspects related to the thermodynamic\ncharacterization of natural gas mixtures blended with hydrogen for the\nintroduction of alternative energy sources within the Power-to-Gas framework.\nFor that purpose, new experimental speed of sound data are presented in the\npressure range between (0.1 up to 13) MPa and at temperatures of (260, 273.16,\n300, 325, and 350) K for two mixtures qualified as primary calibration\nstandards: a 11 component synthetic natural gas mixture (11 M), and another\nlow-calorific $H_{2}$-enriched natural gas mixture with a nominal molar\npercentage $x_{H_{2}}$ = 3%. Measurements have been gathered using a spherical\nacoustic resonator with an experimental expanded ($k$ = 2) uncertainty better\nthan 200 parts in $10^{6}$ (0.02%) in the speed of sound. The heat capacity\nratio as perfect-gas $\\gamma_{pg}$, the molar heat capacity as perfect-gas\n$C_{p,m}^{pg}$, and the second $\\beta_{a}$ and third $\\gamma_{a}$ acoustic\nvirial coefficients are derived from the speed of sound values. All the results\nare compared with the reference mixture models for natural gas-like mixtures,\nthe AGA8-DC92 EoS and the GERG-2008 EoS, with special attention to the impact\nof hydrogen on those properties. Data are found to be mostly consistent within\nthe model uncertainty in the 11 M synthetic mixture as expected, but for the\nhydrogen-enriched mixture in the limit of the model uncertainty at the highest\nmeasuring pressures.","PeriodicalId":501304,"journal":{"name":"arXiv - PHYS - Chemical Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-06","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-2409.04094","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
This work aims to address the technical aspects related to the thermodynamic
characterization of natural gas mixtures blended with hydrogen for the
introduction of alternative energy sources within the Power-to-Gas framework.
For that purpose, new experimental speed of sound data are presented in the
pressure range between (0.1 up to 13) MPa and at temperatures of (260, 273.16,
300, 325, and 350) K for two mixtures qualified as primary calibration
standards: a 11 component synthetic natural gas mixture (11 M), and another
low-calorific $H_{2}$-enriched natural gas mixture with a nominal molar
percentage $x_{H_{2}}$ = 3%. Measurements have been gathered using a spherical
acoustic resonator with an experimental expanded ($k$ = 2) uncertainty better
than 200 parts in $10^{6}$ (0.02%) in the speed of sound. The heat capacity
ratio as perfect-gas $\gamma_{pg}$, the molar heat capacity as perfect-gas
$C_{p,m}^{pg}$, and the second $\beta_{a}$ and third $\gamma_{a}$ acoustic
virial coefficients are derived from the speed of sound values. All the results
are compared with the reference mixture models for natural gas-like mixtures,
the AGA8-DC92 EoS and the GERG-2008 EoS, with special attention to the impact
of hydrogen on those properties. Data are found to be mostly consistent within
the model uncertainty in the 11 M synthetic mixture as expected, but for the
hydrogen-enriched mixture in the limit of the model uncertainty at the highest
measuring pressures.