{"title":"H2/空气火焰-激波相互作用的数值与实验比较","authors":"Emilie Yhuel , Anthony Roque Ccacya , Guillaume Ribert , Pascale Domingo , Nabiha Chaumeix","doi":"10.1016/j.proci.2025.105847","DOIUrl":null,"url":null,"abstract":"<div><div>A high-fidelity three-dimensional numerical simulation is performed to replicate the experimental shock tube setup of the ICARE laboratory, where a hydrogen–air flame–shock interaction (FSI) is studied. Following the experimental procedure, a lean flame (<span><math><mrow><mi>ϕ</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>8</mn></mrow></math></span>) is ignited at the closed end of a rectangular channel before a shock wave, traveling at a Mach number of <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>9</mn></mrow></math></span>, is triggered from the opposite side. The FSI occurs when the shock wave encounters the laminar flame in the visualization window, where experimental schlieren images have been captured. To reproduce this experiment, the fully compressible Navier–Stokes equations are solved using the San Diego mechanism, which includes nine reacting species (excluding nitrogen oxides) and 23 kinetic reactions. Species diffusion is modeled using the Hirschfelder–Curtiss model combined with thermal diffusion (Soret effect). Additionally, gravity is accounted for in the simulation.</div><div>The three major observations of the experiment were well captured by the numerical simulations through a comparison of experimental and numerical schlieren images: the laminar flame propagation and its interaction with adjacent walls; the first FSI, which leads to the formation of Richtmyer–Meshkov instabilities (RMI); and finally, the second FSI, occurring when the reflected shock wave travels back towards the entrance, generating reactive boundary layers and multiple shock interactions within the funnel of fresh gases produced by the RMI.</div></div>","PeriodicalId":408,"journal":{"name":"Proceedings of the Combustion Institute","volume":"41 ","pages":"Article 105847"},"PeriodicalIF":5.2000,"publicationDate":"2025-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Numerical and experimental comparison of H2/air flame–shock interaction\",\"authors\":\"Emilie Yhuel , Anthony Roque Ccacya , Guillaume Ribert , Pascale Domingo , Nabiha Chaumeix\",\"doi\":\"10.1016/j.proci.2025.105847\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>A high-fidelity three-dimensional numerical simulation is performed to replicate the experimental shock tube setup of the ICARE laboratory, where a hydrogen–air flame–shock interaction (FSI) is studied. Following the experimental procedure, a lean flame (<span><math><mrow><mi>ϕ</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>8</mn></mrow></math></span>) is ignited at the closed end of a rectangular channel before a shock wave, traveling at a Mach number of <span><math><mrow><msub><mrow><mi>M</mi></mrow><mrow><mi>s</mi></mrow></msub><mo>=</mo><mn>1</mn><mo>.</mo><mn>9</mn></mrow></math></span>, is triggered from the opposite side. The FSI occurs when the shock wave encounters the laminar flame in the visualization window, where experimental schlieren images have been captured. To reproduce this experiment, the fully compressible Navier–Stokes equations are solved using the San Diego mechanism, which includes nine reacting species (excluding nitrogen oxides) and 23 kinetic reactions. Species diffusion is modeled using the Hirschfelder–Curtiss model combined with thermal diffusion (Soret effect). Additionally, gravity is accounted for in the simulation.</div><div>The three major observations of the experiment were well captured by the numerical simulations through a comparison of experimental and numerical schlieren images: the laminar flame propagation and its interaction with adjacent walls; the first FSI, which leads to the formation of Richtmyer–Meshkov instabilities (RMI); and finally, the second FSI, occurring when the reflected shock wave travels back towards the entrance, generating reactive boundary layers and multiple shock interactions within the funnel of fresh gases produced by the RMI.</div></div>\",\"PeriodicalId\":408,\"journal\":{\"name\":\"Proceedings of the Combustion Institute\",\"volume\":\"41 \",\"pages\":\"Article 105847\"},\"PeriodicalIF\":5.2000,\"publicationDate\":\"2025-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the Combustion Institute\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S1540748925000616\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENERGY & FUELS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the Combustion Institute","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1540748925000616","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
Numerical and experimental comparison of H2/air flame–shock interaction
A high-fidelity three-dimensional numerical simulation is performed to replicate the experimental shock tube setup of the ICARE laboratory, where a hydrogen–air flame–shock interaction (FSI) is studied. Following the experimental procedure, a lean flame () is ignited at the closed end of a rectangular channel before a shock wave, traveling at a Mach number of , is triggered from the opposite side. The FSI occurs when the shock wave encounters the laminar flame in the visualization window, where experimental schlieren images have been captured. To reproduce this experiment, the fully compressible Navier–Stokes equations are solved using the San Diego mechanism, which includes nine reacting species (excluding nitrogen oxides) and 23 kinetic reactions. Species diffusion is modeled using the Hirschfelder–Curtiss model combined with thermal diffusion (Soret effect). Additionally, gravity is accounted for in the simulation.
The three major observations of the experiment were well captured by the numerical simulations through a comparison of experimental and numerical schlieren images: the laminar flame propagation and its interaction with adjacent walls; the first FSI, which leads to the formation of Richtmyer–Meshkov instabilities (RMI); and finally, the second FSI, occurring when the reflected shock wave travels back towards the entrance, generating reactive boundary layers and multiple shock interactions within the funnel of fresh gases produced by the RMI.
期刊介绍:
The Proceedings of the Combustion Institute contains forefront contributions in fundamentals and applications of combustion science. For more than 50 years, the Combustion Institute has served as the peak international society for dissemination of scientific and technical research in the combustion field. In addition to author submissions, the Proceedings of the Combustion Institute includes the Institute''s prestigious invited strategic and topical reviews that represent indispensable resources for emergent research in the field. All papers are subjected to rigorous peer review.
Research papers and invited topical reviews; Reaction Kinetics; Soot, PAH, and other large molecules; Diagnostics; Laminar Flames; Turbulent Flames; Heterogeneous Combustion; Spray and Droplet Combustion; Detonations, Explosions & Supersonic Combustion; Fire Research; Stationary Combustion Systems; IC Engine and Gas Turbine Combustion; New Technology Concepts
The electronic version of Proceedings of the Combustion Institute contains supplemental material such as reaction mechanisms, illustrating movies, and other data.