{"title":"Leakage process and spontaneous ignition of hydrogen within a tube after releasing from the storage container with pressures up to 20 MPa","authors":"Ya-Long Du, Z.Y. Sun, Qin Huang","doi":"10.1016/j.psep.2024.11.041","DOIUrl":null,"url":null,"abstract":"Albeit pressurized storage of gaseous hydrogen is the most common approach to hydrogen storage in the current industry, there is a risk of hydrogen leakage in current metal pipelines, following the potential of hydrogen spontaneous ignition during leakage. Under different burst pressures (from 4 MPa to 20 MPa, corresponding to the actual engineering pressure range in China’s current high/ultra-high-pressure pipelines), the present work investigates the leakage process of hydrogen within a tube by validated models. Hydrogen has been observed to spontaneously ignite when the burst pressure is no less than 4 MPa. The time to spontaneous ignition exponentially declines as burst pressure rises, but it can hardly be reduced to less than 10 μs since a period is required to prepare ignition conditions. Three modes of spontaneous ignition have been classified according to the locations at which initial flame kernels spontaneously appear. Mode I (burst pressure of fewer than 8 MPa) triggers spontaneous ignition near the tube’s wall, Mode III (burst pressure of more than 8 MPa) generates initial flame kernels at the tube’s central axis, while Mode II (burst pressure of 8 MPa) obtains the flame kernels at both locations. At lower burst pressures, the shockwave intensity alone cannot raise the hydrogen-air mixture's temperature to the ignition temperature; the help of boundary layer effects is essential to spontaneous ignition. At higher burst pressures, the shockwave intensity is dominant in raising the hydrogen-air mixture's temperature to reach the ignition condition. Furthermore, tulip flames expand rapidly under high-pressure conditions and form stable structures, indicating pressurized hydrogen exhibits a greater propensity for generating intense flames.","PeriodicalId":20743,"journal":{"name":"Process Safety and Environmental Protection","volume":"190 1","pages":""},"PeriodicalIF":6.9000,"publicationDate":"2024-11-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Process Safety and Environmental Protection","FirstCategoryId":"93","ListUrlMain":"https://doi.org/10.1016/j.psep.2024.11.041","RegionNum":2,"RegionCategory":"环境科学与生态学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, CHEMICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Albeit pressurized storage of gaseous hydrogen is the most common approach to hydrogen storage in the current industry, there is a risk of hydrogen leakage in current metal pipelines, following the potential of hydrogen spontaneous ignition during leakage. Under different burst pressures (from 4 MPa to 20 MPa, corresponding to the actual engineering pressure range in China’s current high/ultra-high-pressure pipelines), the present work investigates the leakage process of hydrogen within a tube by validated models. Hydrogen has been observed to spontaneously ignite when the burst pressure is no less than 4 MPa. The time to spontaneous ignition exponentially declines as burst pressure rises, but it can hardly be reduced to less than 10 μs since a period is required to prepare ignition conditions. Three modes of spontaneous ignition have been classified according to the locations at which initial flame kernels spontaneously appear. Mode I (burst pressure of fewer than 8 MPa) triggers spontaneous ignition near the tube’s wall, Mode III (burst pressure of more than 8 MPa) generates initial flame kernels at the tube’s central axis, while Mode II (burst pressure of 8 MPa) obtains the flame kernels at both locations. At lower burst pressures, the shockwave intensity alone cannot raise the hydrogen-air mixture's temperature to the ignition temperature; the help of boundary layer effects is essential to spontaneous ignition. At higher burst pressures, the shockwave intensity is dominant in raising the hydrogen-air mixture's temperature to reach the ignition condition. Furthermore, tulip flames expand rapidly under high-pressure conditions and form stable structures, indicating pressurized hydrogen exhibits a greater propensity for generating intense flames.
期刊介绍:
The Process Safety and Environmental Protection (PSEP) journal is a leading international publication that focuses on the publication of high-quality, original research papers in the field of engineering, specifically those related to the safety of industrial processes and environmental protection. The journal encourages submissions that present new developments in safety and environmental aspects, particularly those that show how research findings can be applied in process engineering design and practice.
PSEP is particularly interested in research that brings fresh perspectives to established engineering principles, identifies unsolved problems, or suggests directions for future research. The journal also values contributions that push the boundaries of traditional engineering and welcomes multidisciplinary papers.
PSEP's articles are abstracted and indexed by a range of databases and services, which helps to ensure that the journal's research is accessible and recognized in the academic and professional communities. These databases include ANTE, Chemical Abstracts, Chemical Hazards in Industry, Current Contents, Elsevier Engineering Information database, Pascal Francis, Web of Science, Scopus, Engineering Information Database EnCompass LIT (Elsevier), and INSPEC. This wide coverage facilitates the dissemination of the journal's content to a global audience interested in process safety and environmental engineering.