4.7 Article

Effect of crossflow on the air entrainment of propane jet diffusion flames and a modified Froude number

期刊

FUEL
卷 233, 期 -, 页码 454-460

出版社

ELSEVIER SCI LTD
DOI: 10.1016/j.fuel.2018.06.066

关键词

Propane; Entrainment; Jet flame; Cross-flow; Modified Froude number; Reynolds number

资金

  1. National Natural Science Foundation of China [51576186, 51636008]
  2. National Key RD Program [2016YFC0801504]
  3. NSFC-STINT joint project (USTC-Lund University)
  4. Key Research Program of the Chinese Academy of Sciences [QYZDB-SSW-JSC029]
  5. Fundamental Research Funds for the Central Universities [WK2320000034, WK2320000036]
  6. China Postdoctoral Science Foundation [2018M632549]
  7. Open Project Program of State Key Laboratory of Fire Science [HZ2018-KF03]

向作者/读者索取更多资源

Gas leakage fire is increasingly common with urbanization and industrialization. Understanding of the entrainment behavior of the jet flame is significant to improve the fuel security management and fire prevention strategy. Many studies have been done in still air and limited studies have focused on the air entrainment of the jet flame under crossflow. This work firstly deduced an expression of the air entrainment ratio (n) incorporating with the flame length and tilt angle based on the momentum balance and, defined a modified Froude number (Fr*) to explore effects of the inertia force (owing to the fuel jet and crossflow) and the combustion-induced buoyancy. Secondly, experiments of propane jet diffusion flames under crossflow were performed. Fuel jet Reynolds number (Re) and jet-to-crossflow momentum flux ratio (RM) were 310-3305 and 0.004-124, respectively. The flame length divided by Re first increased and then decreased with RM, and its curves were more like parabolas other than polylines. The flame tilt angle decreased with RM. Moreover, Fr* had a negative relationship with RM, indicating the jet and crossflow momenta, instead of combustion-induced buoyancy, gradually dominated the air entrainment with increasing wind velocity. The calculated n was dominated by the flame length but effected by the tilt angle, because the local entrainment velocity was proportional to the magnitudes of the crossflow velocity and flame axial velocity differences that were relevant to the flame tilt angle. Finally, there were three trends of n with Fr* according to Re. For Re < 900, the crossflow was always dominant and n varied slowly. For 900 < Re < 2300, n first grew quickly with stretched and slightly inclined flames and then decreased to some almost constants with nearly horizontal flames. For Re > 2300, n increased rapidly owing to the dominated-effect of the momentum and then decreased until the flame began to shorten.

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