Tomohiko Imamura, O. Sugawa, K. Kamiya, Y. Oka, Toshimitsu Suzuki, Yu-ichi Yamamoto
{"title":"Flame Height of a Turbulent Diffusion Jet Flame with a Comparatively High Initial Discharging Velocity","authors":"Tomohiko Imamura, O. Sugawa, K. Kamiya, Y. Oka, Toshimitsu Suzuki, Yu-ichi Yamamoto","doi":"10.3210/FST.29.15","DOIUrl":null,"url":null,"abstract":"A series of experiments was carried out in order to investigate the visible flame height of a jet flame with a high initial discharging velocity where the fuel-release time and mass flow rate of fuel were varied. The values of non-dimensional heat release rate (Q*) in present experiment were in the range of 107 Q* 8. Even if the value of Q* was larger than 106, when the non-dimensional number (RM) employed by Heskestad which implies the ratio of gas release momentum to the momentum made by a purely buoyant diffusion flame was less than 0.1, the flame height with a comparatively high initial discharging velocity increased with the heat release rate. In other words, whether flame height depends on the Q*2/5 or not can be decided by the range of momentum ratio (RM) regardless of the range of non-dimensional heat release rate (Q*). This can be also decided by the fire Froude number employed by Delichatsios.","PeriodicalId":12289,"journal":{"name":"Fire Science and Technology","volume":"80 1","pages":"15-26"},"PeriodicalIF":0.0000,"publicationDate":"2010-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Fire Science and Technology","FirstCategoryId":"1087","ListUrlMain":"https://doi.org/10.3210/FST.29.15","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
A series of experiments was carried out in order to investigate the visible flame height of a jet flame with a high initial discharging velocity where the fuel-release time and mass flow rate of fuel were varied. The values of non-dimensional heat release rate (Q*) in present experiment were in the range of 107 Q* 8. Even if the value of Q* was larger than 106, when the non-dimensional number (RM) employed by Heskestad which implies the ratio of gas release momentum to the momentum made by a purely buoyant diffusion flame was less than 0.1, the flame height with a comparatively high initial discharging velocity increased with the heat release rate. In other words, whether flame height depends on the Q*2/5 or not can be decided by the range of momentum ratio (RM) regardless of the range of non-dimensional heat release rate (Q*). This can be also decided by the fire Froude number employed by Delichatsios.