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image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Applied Thermal Engi...arrow_drop_down
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
Applied Thermal Engineering
Article . 2016 . Peer-reviewed
License: Elsevier TDM
Data sources: Crossref
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On predicting the length, width, and volume of the jet diffusion flame

Authors: Yang Zhou; Xuanyu Ji; Yangfan Song; Yinhu Kang; Tianfeng Lu; Xiaofeng Lu; Xiaomei Huang; +2 Authors

On predicting the length, width, and volume of the jet diffusion flame

Abstract

Abstract In this paper, the flame length (Lf), width (Wf), and volume (Vf) behaviors of the jet diffusion flame were experimentally and theoretically studied. Various fuel nozzle diameters (df), fuel jet velocities (uf), and air co-flow velocities (uco) were involved in the experiments to investigate their impacts on flame characteristics systematically. Additionally, the analytical solutions for the flow field, fuel concentration, Lf, Wf, and Vf of the jet diffusion flame were derived by theoretical analysis. The results show that flame shape and dimensions of the jet diffusion flame depended on fuel jet Reynolds number (Ref) inherently. At the laminar regime, the dimensionless flame length normalized by df (Lf*) was proportional to Ref. At the laminar–turbulent transitional regime and fully-turbulent regime, Lf* kept nearly constant. The dimensionless flame width (Wf*) remained basically unchanged at the laminar or fully-turbulent regime; but it increased fairly quickly with the increment in Ref at the laminar–turbulent transitional regime. The dimensionless flame volume (Vf*) increased linearly with Ref at the laminar regime, and parabolically with Ref at the laminar–turbulent transitional regime. At the fully-turbulent regime, Vf* kept constant. Besides, with the increase in uco, Lf* maintained nearly unchanged, and Wf* decreased exponentially. Based on the above behaviors, new forms of correlations for Lf*, Wf*, and Vf* of the jet diffusion flame were proposed presently. Comparisons of these correlations with the existing ones in the literature were also conducted in this paper. Moreover, Lf*, Wf*, and Vf* correlations for the dimethyl ether/air jet diffusion flames were developed herein.

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citations
This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
BIP!Impulse provided by BIP!
34
Top 10%
Top 10%
Top 10%