Influence of sub-atmospheric pressure on flame shape and sooting propensity in ethylene laminar coflow non-premixed flame

被引:6
作者
Jalain, R. [1 ,2 ]
Bonnety, J. [1 ,3 ]
Matynia, A. [1 ]
Citerne, J. M. [1 ]
Dutilleul, H. [1 ]
Jocher, A. [4 ]
Consalvi, J. L. [5 ]
Legros, G. [1 ,6 ]
机构
[1] Sorbonne Univ, Inst Jean Rond Alembert, CNRS, UMR 7190, F-75005 Paris, France
[2] Univ Paris Saclay, DMPE, ONERA Palaiseau, F-91123 Palaiseau, France
[3] Univ Paris Saclay, CNRS, Cent Supelec, EM2C, F-91190 Gif sur Yvette, France
[4] Tech Univ Munich, Sch Engn & Design, TUM, Boltzmann Str 15, D-85748 Garching, Germany
[5] Aix Marseille Univ, IUSTI UMR, CNRS 7343, 5 Rue E Fermi, F-13453 Marseille 13, France
[6] Univ Orleans, CNRS ICARE, 1C Ave Rech Sci, F-45071 Orleans 2, France
关键词
Optical diagnostics; Sub-atmospheric pressure; Sooting non-premixed flame; TEMPERATURE-FIELD STRUCTURE; AIR DIFFUSION FLAMES; OXIDATION; METHANE; DEPENDENCE; ETHANE; TRANSITION; SIMULATION; PYROMETRY; SURFACE;
D O I
10.1016/j.combustflame.2023.113173
中图分类号
O414.1 [热力学];
学科分类号
摘要
Sooting flames have been a longstanding research topic and an extensive literature has been developed at both atmospheric and high pressure. In contrast, studies of sooting flames at subatmospheric pressures are relatively scarce. As pressure decreases buoyancy, and consequently buoyancy-driven convective flow, decreases as well. So one could expect characteristic residence times to be longer. To assess the intuitive finding, steady coflow non-premixed ethylene/air flames were established at different pressure conditions, ranging from 0.2 to 1 bar. The configuration was documented by both numerical and experimental works. By the Modulated Absorption Emission (MAE) technique, fields of temperature, soot volume fraction, and dispersion exponent as a measure of soot maturity were extracted. Extending the MAE setup from 2 to 4 spectral ranges allows a more accurate evaluation of the dispersion exponent together with the temperature calibration factor. Numerical simulations were conducted using the CoFlame code, giving access to the flow topology and the governing characteristic times. According to numerical simulations, with increasing pressure, while the buoyancy-driven convective flow does increase, the flow velocities do decrease. It seems consistent with experimental results, finding higher maturity, expected with higher residence time, when increasing pressure. In addition to the important database produced for flames under sub-atmospheric conditions, this paper also couples originally experimental and numerical results, leading to (i) the reconstruction of the synthetic signals that a camera would capture, and (ii) the tracking of the quantities of interest experienced along the streamlines. Most of the global trends are well-captured by CoFlame, i.e. decreasing pressure leads to the decrease of soot volume fraction, maturity, and flame height, together with the increase in temperature. Meanwhile, significant discrepancies can be noticed, i.e. the numerical simulations overestimate the soot volume fraction, especially for the lower pressure levels, together with an underestimated flame temperature leading to an overestimation of the flame height.
引用
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页数:13
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共 66 条
[1]   Kinetic modeling of soot formation with detailed chemistry and physics:: Laminar premixed flames of C2 hydrocarbons [J].
Appel, J ;
Bockhorn, H ;
Frenklach, M .
COMBUSTION AND FLAME, 2000, 121 (1-2) :122-136
[2]   A novel soot model for fires: Validation in a laminar non-premixed flame [J].
Beji, T. ;
Zhang, J. P. ;
Yao, W. ;
Delichatsios, M. .
COMBUSTION AND FLAME, 2011, 158 (02) :281-290
[3]   Soot formation and temperature field structure in laminar propane-air diffusion flames at elevated pressures [J].
Bento, Decio S. ;
Thomson, Kevin A. ;
Gulder, Omer L. .
COMBUSTION AND FLAME, 2006, 145 (04) :765-778
[4]   Analyzing the effects of temperature on soot formation with a joint volume-surface-hydrogen model [J].
Blanquart, G. ;
Pitsch, H. .
COMBUSTION AND FLAME, 2009, 156 (08) :1614-1626
[5]   Probing the local radiative quenching during the transition from a non-smoking to a smoking laminar coflow ethylene/air non-premixed flame [J].
Bonnety, Jerome ;
Guibaud, Augustin ;
Jalain, Renaud ;
Matynia, Alexis ;
Consalvi, Jean-Louis ;
Liu, Fengshan ;
Legros, Guillaume .
COMBUSTION AND FLAME, 2019, 203 :120-129
[6]   Predictions of soot and thermal radiation properties in confined turbulent jet diffusion flames [J].
Brookes, SJ ;
Moss, JB .
COMBUSTION AND FLAME, 1999, 116 (04) :486-503
[7]   Kinetics of nascent soot oxidation by molecular oxygen in a flow reactor [J].
Camacho, Joaquin ;
Tao, Yujie ;
Wang, Hai .
PROCEEDINGS OF THE COMBUSTION INSTITUTE, 2015, 35 :1887-1894
[8]   DETERMINATION OF THE WAVELENGTH DEPENDENCE OF REFRACTIVE-INDEXES OF FLAME SOOT [J].
CHANG, H ;
CHARALAMPOPOULOS, TT .
PROCEEDINGS OF THE ROYAL SOCIETY-MATHEMATICAL AND PHYSICAL SCIENCES, 1990, 430 (1880) :577-591
[9]   A numerical study on the effects of pressure and gravity in laminar ethylene diffusion flames [J].
Charest, Marc R. J. ;
Groth, Clinton P. T. ;
Guelder, Oemer L. .
COMBUSTION AND FLAME, 2011, 158 (10) :1933-1945
[10]   Effects of gravity and pressure on laminar coflow methane-air diffusion flames at pressures from 1 to 60 atmospheres [J].
Charest, Marc R. J. ;
Groth, Clinton P. T. ;
Guelder, Oemer L. .
COMBUSTION AND FLAME, 2011, 158 (05) :860-875