2016
DOI: 10.1016/j.ijhydene.2016.02.151
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Experimental and theoretical analysis of cellular instability in lean H 2 -CH 4 -air flames at elevated pressures

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Cited by 71 publications
(10 citation statements)
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“…The first is dominated by the adiabatic explosion pressure, while the latter is related to the propagation speed of the blast wave during explosion. Different to other fuels, hydrogen gas has a stronger diffusion-thermal characteristic [16][17][18][19], which makes the values of adiabatic explosion pressure close for the case of the stoichiometric and φ = 1.2 levels, obviously higher than those in the cases whose equivalence ratio outside the range of 1.0-1.2 and, thus, it results in p max being attained in the case of φ = 1.0-1.2. However, like most practical thermal or power devices, the explosion vessel is not an adiabatic system and certain amounts of released heat is lost during the explosion process for the temperature drop across the vessel's wall and, resultantly, the actual value of p max is less than the adiabatic explosion pressure.…”
Section: Resultsmentioning
confidence: 99%
“…The first is dominated by the adiabatic explosion pressure, while the latter is related to the propagation speed of the blast wave during explosion. Different to other fuels, hydrogen gas has a stronger diffusion-thermal characteristic [16][17][18][19], which makes the values of adiabatic explosion pressure close for the case of the stoichiometric and φ = 1.2 levels, obviously higher than those in the cases whose equivalence ratio outside the range of 1.0-1.2 and, thus, it results in p max being attained in the case of φ = 1.0-1.2. However, like most practical thermal or power devices, the explosion vessel is not an adiabatic system and certain amounts of released heat is lost during the explosion process for the temperature drop across the vessel's wall and, resultantly, the actual value of p max is less than the adiabatic explosion pressure.…”
Section: Resultsmentioning
confidence: 99%
“…The flames can be observed in the chamber through the optical windows up to a diameter of 60 mm. The flames propagated at constant pressure from the time of ignition until their diameter was about 60 mm [26][27][28].…”
Section: Experimental Setup and Conditionsmentioning
confidence: 99%
“…The relationship between flame speed, Sn, and flame stretch rate, α, is given in Figure 3. Unstretched laminar burning velocity, SL, evaluations were conducted with Equation 6where ρ u and ρ b are unburnt mixture and burnt gas density, respectively [5,17,24,28]. Figure 5, the solid lines show the experimental results while the dashed lines show the outcome of numerical investigation using CHEMKIN-PRO.…”
Section: Experimental Setup and Conditionsmentioning
confidence: 99%
“…Cellular structures formed on the flame front increase the flame surface area and cause flame self-acceleration [26]. In this regard, Markstein length and cellular instability for various fuel/oxidizer mixtures have been studied extensively [27][28][29][30][31]. Laminar flame characteristics of butanol have been widely studied by various methods of experimental measurement and mechanism prediction [24,32,33].…”
Section: Introductionmentioning
confidence: 99%