Biogas Laminar Burning Velocity and Flammability Characteristics in Spark Ignited Premix Combustion

被引:17
作者
Anggono, Willyanto [1 ,2 ,3 ]
Wardana, I. N. G. [2 ]
Lawes, M. [4 ]
Hughes, K. J. [3 ]
Wahyudi, Slamet [2 ]
Hamidi, Nurkholis [2 ]
Hayakawa, Akihiro [5 ]
机构
[1] Petra Christian Univ, Dept Mech Engn, Surabaya, Indonesia
[2] Brawijaya Univ, Doctoral Program Mech Engn Dept, Malang, Indonesia
[3] Univ Leeds, Sch Proc, Environm & Mat Engn, Leeds LS2 9JT, W Yorkshire, England
[4] Univ Leeds, Sch Mech Engn, Leeds LS2 9JT, W Yorkshire, England
[5] Kyushu Univ, Dept Mech Engn, Fukuoka, Japan
来源
2013 INTERNATIONAL CONFERENCE ON SCIENCE & ENGINEERING IN MATHEMATICS, CHEMISTRY AND PHYSICS (SCIETECH 2013) | 2013年 / 423卷
关键词
PRODUCER GAS; AIR MIXTURES; ENGINE; TEMPERATURES; PRESSURES; METHANE; FUEL;
D O I
10.1088/1742-6596/423/1/012015
中图分类号
O69 [应用化学];
学科分类号
081704 ;
摘要
Spherically expanding flames propagating at constant pressure were employed to determine the laminar burning velocity and flammability characteristics of biogas-air mixtures in premixed combustion to uncover the fundamental flame propagation characteristics of a new alternative and renewable fuel. The results are compared with those from a methane-air flame. Biogas is a sustainable and renewable fuel that is produced in digestion facilities. The composition of biogas discussed in this paper consists of 66.4% methane, 30.6% carbon dioxide and 3% nitrogen. Burning velocity was measured at various equivalence ratios (phi) using a photographic technique in a high pressure fan-stirred bomb, the initial condition being at room temperature and atmospheric pressure. The flame for methane-air mixtures propagates from phi=0.6 till phi=1.3. The flame at phi >= 1.4 does not propagate because the combustion reaction is quenched by the larger mass of fuel. At phi <= 0.5, it does not propagate as well since the heat of reaction is insufficient to burn the mixtures. The flame for biogas-air mixtures propagates in a narrower range, that is from phi=0.6 to phi=1.2. Different from the methane flame, the biogas flame does not propagate at phi >= 1.3 because the heat absorbed by inhibitors strengthens the quenching effect by the larger mass of fuel. As in the methane flame, the biogas flame at phi <= 0.5 does not propagate. This shows that the effect of inhibitors in extremely lean mixtures is small. Compared to a methane-air mixture, the flammability characteristic (flammable region) of biogas becomes narrower in the presence of inhibitors (carbon dioxide and nitrogen) and the presence of inhibitors causes a reduction in the laminar burning velocity. The inhibitor gases work more effectively at rich mixtures because the rich biogas-air mixtures have a higher fraction of carbon dioxide and nitrogen components compared to the lean biogas-air mixtures.
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页数:7
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