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Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility

A thermochemical nonequilibrium analysis was performed under the low enthalpy shock-tunnel flows. A quasi-one-dimensional flow calculation was employed by dividing the flow calculations into two parts, for the shock-tube and the Mach 6 nozzle. To describe the thermochemical nonequilibrium of the low...

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Autores principales: Lee, Sanghoon, Kim, Ikhyun, Park, Gisu, Lee, Jong Kook, Kim, Jae Gang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Public Library of Science 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7540898/
https://www.ncbi.nlm.nih.gov/pubmed/33027277
http://dx.doi.org/10.1371/journal.pone.0240300
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author Lee, Sanghoon
Kim, Ikhyun
Park, Gisu
Lee, Jong Kook
Kim, Jae Gang
author_facet Lee, Sanghoon
Kim, Ikhyun
Park, Gisu
Lee, Jong Kook
Kim, Jae Gang
author_sort Lee, Sanghoon
collection PubMed
description A thermochemical nonequilibrium analysis was performed under the low enthalpy shock-tunnel flows. A quasi-one-dimensional flow calculation was employed by dividing the flow calculations into two parts, for the shock-tube and the Mach 6 nozzle. To describe the thermochemical nonequilibrium of the low enthalpy shock-tunnel flows, a three-temperature model is proposed. The three-temperature model treats the vibrational nonequilibrium of O(2) and NO separately from the single nonequilibrium energy mode of the previous two-temperature model. In the three-temperature model, electron-electronic energies and vibrational energy of N(2) are grouped as one energy mode, and vibrational energies of O(2), O(2)(+), and NO are grouped as another energy mode. The results for the shock-tunnel flows calculated using the three-temperature model were then compared with existing experimental data and the results obtained from one- and two-temperature models, for various operating conditions of the K1 shock-tunnel facility. The results of the thermochemical nonequilibrium analysis of the low enthalpy shock-tunnel flows suggest that the nonequilibrium characteristics of N(2) and O(2) need to be treated separately. The vibrational relaxation of O(2) is much faster than that of N(2) in low enthalpy condition, and the dissociation rate of O(2) is manly influenced by the species vibrational temperature of O(2). The proposed three-temperature model is able to describe the thermochemical nonequilibrium characteristics of N(2) and O(2) behind the incident and reflected shock waves, and the rapid vibrational freezing of N(2) in nozzle expanding flows.
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spelling pubmed-75408982020-10-19 Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility Lee, Sanghoon Kim, Ikhyun Park, Gisu Lee, Jong Kook Kim, Jae Gang PLoS One Research Article A thermochemical nonequilibrium analysis was performed under the low enthalpy shock-tunnel flows. A quasi-one-dimensional flow calculation was employed by dividing the flow calculations into two parts, for the shock-tube and the Mach 6 nozzle. To describe the thermochemical nonequilibrium of the low enthalpy shock-tunnel flows, a three-temperature model is proposed. The three-temperature model treats the vibrational nonequilibrium of O(2) and NO separately from the single nonequilibrium energy mode of the previous two-temperature model. In the three-temperature model, electron-electronic energies and vibrational energy of N(2) are grouped as one energy mode, and vibrational energies of O(2), O(2)(+), and NO are grouped as another energy mode. The results for the shock-tunnel flows calculated using the three-temperature model were then compared with existing experimental data and the results obtained from one- and two-temperature models, for various operating conditions of the K1 shock-tunnel facility. The results of the thermochemical nonequilibrium analysis of the low enthalpy shock-tunnel flows suggest that the nonequilibrium characteristics of N(2) and O(2) need to be treated separately. The vibrational relaxation of O(2) is much faster than that of N(2) in low enthalpy condition, and the dissociation rate of O(2) is manly influenced by the species vibrational temperature of O(2). The proposed three-temperature model is able to describe the thermochemical nonequilibrium characteristics of N(2) and O(2) behind the incident and reflected shock waves, and the rapid vibrational freezing of N(2) in nozzle expanding flows. Public Library of Science 2020-10-07 /pmc/articles/PMC7540898/ /pubmed/33027277 http://dx.doi.org/10.1371/journal.pone.0240300 Text en © 2020 Lee et al http://creativecommons.org/licenses/by/4.0/ This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/) , which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
spellingShingle Research Article
Lee, Sanghoon
Kim, Ikhyun
Park, Gisu
Lee, Jong Kook
Kim, Jae Gang
Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title_full Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title_fullStr Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title_full_unstemmed Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title_short Thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
title_sort thermochemical nonequilibrium flow analysis in low enthalpy shock-tunnel facility
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7540898/
https://www.ncbi.nlm.nih.gov/pubmed/33027277
http://dx.doi.org/10.1371/journal.pone.0240300
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