Home > CSC-OpenAccess Library > Manuscript Information
EXPLORE PUBLICATIONS BY COUNTRIES |
EUROPE | |
MIDDLE EAST | |
ASIA | |
AFRICA | |
............................. | |
United States of America | |
United Kingdom | |
Canada | |
Australia | |
Italy | |
France | |
Brazil | |
Germany | |
Malaysia | |
Turkey | |
China | |
Taiwan | |
Japan | |
Saudi Arabia | |
Jordan | |
Egypt | |
United Arab Emirates | |
India | |
Nigeria |
Experimental Investigation of Flame Kernel in Turbulent Partial Premixed Flames
A. M. Elbaz, Mohy Mansour, Diaaeldin Mohamed
Pages - 21 - 34 | Revised - 15-11-2012 | Published - 31-12-2012
Published in International Journal of Applied Sciences (IJAS)
MORE INFORMATION
KEYWORDS
Flame kernel, Partial premixed flame, PIV, Flow field
ABSTRACT
The flame kernel propagation is believed to be influenced by many operating parameters such as mixing level, turbulent intensity, and the mixture equivalence ratio. The purpose of this study is to investigate the effect of the mixture equivalence ratio and turbulence intensity on the flame kernel and flow field interlinks in partially premixed natural gas flames. Three jet equivalence ratios of 1, 1.5, and 2 are considered at values of jet velocities in the range from 10 to 20 m/s. This study was done under constant degree of partial premixing. A pulsed Nd: YAG laser is used for the flame ignition, and the turbulent flow field is captured at several time intervals from ignition using two-dimensional Planar Imaging Velocimetry (PIV). The mean flow field doesn’t influence with the flame kernel propagation. The turbulent flow field indicates an increase in the global turbulence intensity in flames associated with the kernel propagation in comparison with the isothermal case. The jet equivalence ratio of one enhances the flame kernel propagation and it gives the highest rate of kernel propagation. Increasing the jet equivalence ratio to 1.5 and 2 reduces the intensity of chemical reaction and hence the effect of turbulence becomes the dominant factor effecting the propagation of the flame kernel .At jet velocity of 20 m/s , an early flame kernel extinction is recorded without any respect to jet equivalence ratio. At the early stage of the kernel generation at delay time of 150 ?s, linear correlation between the jet velocity and the kernel propagation is noticed. The chemical reaction is the main factor influences the rate of kernel propagation; it gives nearly 3.5 times the effect of the flow convection to the maximum rate of the flame kernel propagation at jet velocity of 20 m/s and equivalence ratio of one.
1 | Mansour, M. S., Elbaz, A. M., & Zayed, M. F. (2014). Flame Kernel Generation and Propagation in Turbulent Partially Premixed Hydrocarbon Jet. Combustion Science and Technology, 186(4-5), 698-711. |
2 | Elbaz, A. M., Mansour, M., Elsayed, K. A., & Mohamed, D. (2013). An experimental study of the effect of partial premixing level on the interaction between the flame kernel and flow field. International Journal of Applied, 4(1), 10. |
A. Dreizler, S. Lindenmaier, U. Maas, J. Hult, M. Alden, C.F. Kaminski, "Characterization of a spark ignition system by planar laser induced fluorescence of high repetition rates and comparison with chemical kinetic calculations," Applied Physics B70:287–294 (2000). | |
B.D. Videto, D.A. Santavicca, "A turbulent flow system for studying turbulent combustion processes,"Combustion Science and Technology 76 (1991) 159–164. | |
C. Arcoumanis, D.R. Hall, and J. H. Whitelaw, "An approach to charge stratification in lean-burn spark-ignition engines," SAE technical paper 941878 (1994). | |
C. Arcoumanis, D.R. Hall, and J.H. Whitelaw, "Optimizing local charge stratification in a lean-burn spark ignition engine," Proc. Instn. Mech. Engrs, Part D: J. Auto. Eng. 211:145–154(1997). | |
C. Arcoumanis, M.R. Gold, J.H. Whitelaw, and H.M. Xu, "Local mixture injection to extend the lean limit of spark-ignition engines," Exper. Fluids 26:126–135 (1999). | |
C.C. Huang, S.S. Shy, C.C. Liu, A. Yan, "A transition on minimum ignition energy for lean turbulent methane combustion in flamelet and distributed regimes," Proceedings of the Combustion Institute 31:1401–1409(2007). | |
C.F. Kaminski, J. Hult, M. Alden, S. Lindenmaier, A. Dreizler, U. Mass, M. Baum, "Complex turbulence/chemistry interactions revealed by time resolved fluorescence and direct numerical simulations," Proceedings of the Combustion Institute 28:399–405(2000). | |
D. Thevenin, O. Gicquel, J. de Charentenay, R. Hilbert, D. Veynante, "Two versus three dimensional direct simulations of turbulent methane flame kernels using realistic chemistry," Proceedings of the Combustion Institute 29:2031–2039 (2003). | |
D. Thevenin, P.H. Renard, J.C. Rolon, and S. Candel, "Extinction processes during a non-premixed flame / vortex interaction," Proceedings of the Combustion Institute. 27:719–726 (1998). | |
D.A. Eichenberger, W.L. Roberts, "Effect of unsteady stretch on spark-ignited flame kernel survival,"Combustion and Flame 118:469–478(1999). | |
G. Patnaik, and K. Kailasanath, "A computational study of local quenching in flame-vortex interactions with radiative losses," Proceedings of the Combustion Institute. 27:711–717 (1998). | |
H. Reddy and J. Abraham, "A Numerical Study of Vortex Interactions with Flames Developing from Ignition Kernels in Lean Methane/Air Mixtures," Combustion and Flame 158 (2011) 401–415. | |
K.W. Jenkins, M. Klein, N. Chakraborty, R.S. Cant, "Effects of strain rate and curvature on the propagation of a spherical flame kernel in the thin reaction zones regime," Combustion and Flame 145:415–434 (2006). | |
K.W. Jenkins, R.S. Cant, "Curvature effects on flame kernels in a turbulent environment," Proceedings of the Combustion Institute 29:2023–2029(2002). | |
M.S. Mansour, , N. Peters, L.U. Schrader, "Experimental study of turbulent flame kernel propagation,"Experimental Thermal and Fluid Science. 32:1396–1404(2008). | |
N. Chakraborty, M. Klein, R.S. Cant, "Stretch effects on displacement speed in turbulent premixed flame kernels in the thin reaction zones regime," Proceedings of the Combustion Institute 31: 1385–1392(2007). | |
P.H. Renard, J.C. Rolon, D. Thevenin, , and S. Candel, "Investigations of heat release, extinction,and time evolution of the flame surface, for a non-premixed flame interacting with a vortex,"Combustion and Flame 117:189–205 (1999). | |
P.H. Renard, J.C. Rolon, D. Thevenin, and S. Candel, "Wrinkling, pocket formation and double premixed flame interaction processes," Proceedings of the Combustion Institute. 27:659–666 (1998). | |
R.R. Maly, in: J.C. Hilliard, G.S. Springer (Eds.), "Flow and Combustion in Reciprocating Engines,"Plenum Press, New York, 1983. | |
S. Gashi, J. Hult, K.W. Jenkins, N. Chakraborty, R.S. Cant, C.F.Kaminski, "Curvature and wrinkling of premixed flame kernels – comparisons of OH PLIF and DNS data," Proceedings of Combustion Institute 30:809–817 (2005). | |
S.K. Marley, S.J. Danby, W.L. Roberts, M.C. Drake, T.D. Fansler, "Quantification of transient stretch effects on kernel–vortex interactions in premixed methane–air flames," Combustion and Flame 154(2008) 296–309. | |
V.R. Katta, K.Y. Iisu, and W.M. Roquemore, "Local Extinction in an unsteady methane-air jet diffusion flame," Proceedings of the Combustion Institute 27:1121-1129 (1998). | |
Y. Xiong, W.L. Roberts, "Observations on the interaction between a premixed flame kernel and a vortex of different equivalence ratio," Proceedings of the Combustion Institute. 29:1687–1693(2002). | |
Y. Xiong, W.L. Roberts, M.C. Drake, T.D. Fansler, "Investigation of pre-mixed flame-kernel/vortex interactions via high-speed imaging," Combustion and Flame 126:1827–1844 (2001). | |
Dr. A. M. Elbaz
Faculty of Engineering/Mechanical Power Engineering Department, Helwan University, Cairo, Egypt - Egypt
aymanelbaz22@gmail.com
Professor Mohy Mansour
Faculty of Engineering/Mechanical Power Engineering Department, Cairo University, Egypt - Egypt
Mr. Diaaeldin Mohamed
Faculty of Engineering/Mechanical Power Engineering Department, Cairo, University, Egypt - Egypt
|
|
|
|
View all special issues >> | |
|
|