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Research Article

Effects of Key Influencing Factors on the Flame Inclination of Low Concentration Methane (LCM) Combustion in Porous Burner

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Pages 4032-4052 | Received 31 Dec 2021, Accepted 14 Mar 2022, Published online: 21 Mar 2022
 

ABSTRACT

In present work, a local thermal non-equilibrium numerical model of low concentration methane combustion in porous media is established. The modified thermal effective thermal conductivity of foam ceramics was introduced. The heat and mass dispersion effect as well as the influence of porous media structure on the heat transfer were fully considered. Studies found that the combustion flame front of low concentration methane in porous media always show a S-shaped state under special conditions. The influencing factors of inlet velocity, methane concentration, wall heat loss, and the porous burner size were analyzed. Results show that without initial thermal perturbation and the absence of defects in the porous media, the flame front in porous burner still has the possibility of inclination. As the inclination of the flame front continues to increase, the flame keeps approaching the burner outlet until blow off. Among the considered four influencing factors, the size of porous burner has the greatest influence on the inclination of flame front. As the burner diameter increases from 0.04 m to 0.12 m, the inclination angle of the flame front increases continuously, and the maximum inclination angle is 36°. The flame inclination will cause uneven temperature distribution downstream of the burner and local heat concentration. With the increase of wall heat loss, the high-temperature zone downstream of the burner will evolve into a local high-temperature zone near the flame front. With the reducing of porous burner diameter, the inclinational instability could be suppressed to some extent.

Nomenclature

Disclosure statement

The authors declare that there is no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Additional information

Funding

Financial supports from the National Natural Science Foundation of China (No. 52174214, 51974303), Key R&D Program of Jiangsu Province (Grant No. BE2020645) and the Fundamental Research Funds for the Central Universities (No. 2020ZDPY0202, No. 2021GJZPY11, No. 2021YCPY0207) are sincerely acknowledged.

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