Abstract:We experimentally studied and kinetically modeled the effects of hydrogen addition on soot formation in methane and ethylene counterflow diffusion flames (CDFs). To isolate the chemical effects of hydrogen in such flames, we also ran a set of experiments on flames of the same base fuels but with the addition of helium. Specifically, we measured the soot volume fractions of the flames using the planar laser-induced incandescence technique. We simulated detailed sooting structures by coupling the gas-phase chemi… Show more
“…It is also noticed that the overall SVF profile seems symmetric under the present X F /X O conditions. This situation is slightly different from the previous CDFs [44] (e.g., with X F = 1.0 and X O = 0.24), in which a skewed shape of the SVF profile (towards the fuel side) was observed. This is because the variations in the flame boundary conditions (X F /X O ) will alter the relative location of the flame sheet to the stagnation plane, which, in turn, will notably affect the soot evolution process and result in different axial distributions of SVF.…”
Section: General Flame Structure Of the Present Counterflow Flamescontrasting
Furanic biofuels have received increasing research interest over recent years, due to their potential in reducing greenhouse gas emissions and mitigating the production of harmful pollutants. Nevertheless, the heterocyclic structure in furans make them readily to produce soot, which requires an in-depth understanding. In this study, the sooting characteristic of several typical furanic biofuels, i.e., furan, 2-methylfuran (MF), and 2,5-dimethylfuran (DMF), were investigated in laminar counterflow flames. Combined laser-based soot measurements with numerical analysis were performed. Special focus was put on understanding how the fuel structure of furans could affect soot formation. The results show that furan has the lowest soot volume fraction, followed by DMF, while MF has the largest value. Kinetic analyses revealed that the decomposition of MF produces high amounts of C3 species, which are efficient benzene precursors. This may be the reason for the enhanced formation of polycyclic aromatic hydrocarbons (PAHs) and soot in MF flames, as compared to DMF and furan flames. The major objectives of this work are to: (1) understand the sooting behavior of furanic fuels in counterflow flames, (2) elucidate the fuel structure effects of furans on soot formation, and (3) provide database of quantitative soot concentration for model validation and refinements.
“…It is also noticed that the overall SVF profile seems symmetric under the present X F /X O conditions. This situation is slightly different from the previous CDFs [44] (e.g., with X F = 1.0 and X O = 0.24), in which a skewed shape of the SVF profile (towards the fuel side) was observed. This is because the variations in the flame boundary conditions (X F /X O ) will alter the relative location of the flame sheet to the stagnation plane, which, in turn, will notably affect the soot evolution process and result in different axial distributions of SVF.…”
Section: General Flame Structure Of the Present Counterflow Flamescontrasting
Furanic biofuels have received increasing research interest over recent years, due to their potential in reducing greenhouse gas emissions and mitigating the production of harmful pollutants. Nevertheless, the heterocyclic structure in furans make them readily to produce soot, which requires an in-depth understanding. In this study, the sooting characteristic of several typical furanic biofuels, i.e., furan, 2-methylfuran (MF), and 2,5-dimethylfuran (DMF), were investigated in laminar counterflow flames. Combined laser-based soot measurements with numerical analysis were performed. Special focus was put on understanding how the fuel structure of furans could affect soot formation. The results show that furan has the lowest soot volume fraction, followed by DMF, while MF has the largest value. Kinetic analyses revealed that the decomposition of MF produces high amounts of C3 species, which are efficient benzene precursors. This may be the reason for the enhanced formation of polycyclic aromatic hydrocarbons (PAHs) and soot in MF flames, as compared to DMF and furan flames. The major objectives of this work are to: (1) understand the sooting behavior of furanic fuels in counterflow flames, (2) elucidate the fuel structure effects of furans on soot formation, and (3) provide database of quantitative soot concentration for model validation and refinements.
“…The impact of H 2 on the formation of soot precursors and soot particles have also been the subject of numerous fundamental studies but mostly for mixtures of H 2 with fuels other than CH 4 [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37]. By contrast, only a few similar studies, to the best of our knowledge, were addressed to characterize the impact of H 2 on the combustion of CH 4 flames [38][39][40][41]. Liu et al [38] and Xu et al [39] studied the effects of H 2 as a fuel additive (up to 40% comparing to the base fuel) on soot formation in diffusion CH 4 flames and showed that the addition of H 2 strongly decreases the formation of soot.…”
Section: Introductionmentioning
confidence: 99%
“…By contrast, only a few similar studies, to the best of our knowledge, were addressed to characterize the impact of H 2 on the combustion of CH 4 flames [38][39][40][41]. Liu et al [38] and Xu et al [39] studied the effects of H 2 as a fuel additive (up to 40% comparing to the base fuel) on soot formation in diffusion CH 4 flames and showed that the addition of H 2 strongly decreases the formation of soot. Ezenwajiaku et al [41] also investigated the impact of H 2 (added up to 20% in CH 4 ) on the formation of PAHs also in a diffusion flame.…”
We report here the experimental investigation of lightly sooting methane premixed flames with and without hydrogen. Two different approaches were considered to introduce hydrogen in the methane flame, either by keeping the total gas flow rate constant or not. Speciation data were obtained using a set of analytical tools including Gas Chromatography, Fourier-Transform Infrared Spectroscopy, Jet-Cooled Laser-Induced Fluorescence, Laser-induced Incandescence coupled with Cavity Ring-Down Spectroscopy.The results include mole fraction profiles of gaseous species (C 0 -C 16 ) and soot volume fraction (f v ) measured in all studied flames. These results demonstrate that the introduction of hydrogen to the flame insignificantly impacts the maximum mole fractions of small species (
“…Regarding the LII setup, a 10 Hz pulsed Nd-YAG laser with a fundamental emission at 1064 nm was used [ 50 , 59 , 60 ]. The laser beam was manipulated by a series of cylindrical lens to form a laser sheet (8 mm high) at the burner center.…”
Highlights
Sooting tendencies rankings among different fuels depend on flame conditions.
Sooting limits of C
5
–C
8
n-alkane is comparable, regardless of carbon-chain length.
Effects of branched fuel structures on sooting tendency kinetically explained.
Cyclopentane has even stronger sooting propensity than cyclohexane.
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