TY - JOUR
T1 - Flame structure and kinetic studies of carbon dioxide-diluted dimethyl ether flames at reduced and elevated pressures
AU - Liu, Dong
AU - Santner, Jeffrey
AU - Togbé, Casimir
AU - Felsmann, Daniel
AU - Koppmann, Julia
AU - Lackner, Alexander
AU - Yang, Xueliang
AU - Shen, Xiaobo
AU - Ju, Yiguang
AU - Kohse-Höinghaus, Katharina
N1 - Funding Information:
D.L. and C.T. thank the Alexander von Humboldt foundation for their research fellowships. The authors thank Wayne Metcalfe, Sinead Burke, Syed Ahmed, and Henry Curran for the use of their unpublished kinetic model. They are also grateful to Stephen Klippenstein for his reaction rate recommendations and to Pascal Diévart for assistance in modeling. They also thank Patrick Nau for his assistance with the exhaust gas temperature measurements for low-pressure flames as well as Regine Schröder for her capable assistance with the redaction of the manuscript. Y.J. would like to thank for the support from the US Department of Energy, Office of Basic Energy Sciences as part of an Energy Frontier Research Center on Combustion with Grant No. DE-SC0001198 and the Alexander von Humboldt foundation for a Friedrich-Wilhelm-Bessel Award. K.K.H. gratefully acknowledges support by the Deutsche Forschungsgemeinschaft within SFB 686 “Model-Based Control of Homogenized Low-Temperature Combustion”, TP B3.
PY - 2013
Y1 - 2013
N2 - The flame structure and kinetics of dimethyl ether (DME) flames with and without CO2 dilution at reduced and elevated pressures were studied experimentally and computationally. The species distributions of DME oxidation in low-pressure premixed flat flames were measured by using electron-ionization molecular-beam mass spectrometry (EI-MBMS) at an equivalence ratio of 1.63 and 50mbar. High-pressure flame speeds of lean and rich DME flames with and without CO2 dilution were measured in a nearly-constant-pressure vessel between about 1 and 20bar. The experimental results were compared with predictions from four kinetic models: the first was published by Zhao et al. (2008) [9], the second developed by the Lawrence Livermore National Laboratory (LLNL) (Kaiser et al., 2000) [13], and the third has been made available to us as the Aramco mechanism (Metcalfe et al., 2013) [14]; as the fourth, we have used an updated model developed in this study. Good agreement was found between measurements and predictions from all four models for all major and most typical intermediate species with and without CO2 addition in low-pressure flat flame experiments. However, none of the models was able to reliably predict high-pressure flame speeds. Although the updated model improved the prediction of flame speeds for lean mixtures, errors remained for rich conditions at elevated pressure, likely due to uncertainty in the rates of CH3+H(+M)=CH4(+M) and the branching and termination reaction pair of CH3+HO2=CH3O+OH and CH3+HO2=CH4+O2. CO2 addition considerably decreased the flame speed. Kinetic comparisons between inert and chemically active CO2 in DME flames showed that CO2 addition affects rich and lean DME flame kinetics differently. For lean flames, both the inert third-body effect and the kinetic effect of CO2 reduce H-atom production. However, for rich flames, the inert third-body effect increases H-atom production via HCO(+M)=H+CO(+M) and suppression of the kinetic effect of CO2 by shifting the equilibrium of CO+OH=CO2+H.
AB - The flame structure and kinetics of dimethyl ether (DME) flames with and without CO2 dilution at reduced and elevated pressures were studied experimentally and computationally. The species distributions of DME oxidation in low-pressure premixed flat flames were measured by using electron-ionization molecular-beam mass spectrometry (EI-MBMS) at an equivalence ratio of 1.63 and 50mbar. High-pressure flame speeds of lean and rich DME flames with and without CO2 dilution were measured in a nearly-constant-pressure vessel between about 1 and 20bar. The experimental results were compared with predictions from four kinetic models: the first was published by Zhao et al. (2008) [9], the second developed by the Lawrence Livermore National Laboratory (LLNL) (Kaiser et al., 2000) [13], and the third has been made available to us as the Aramco mechanism (Metcalfe et al., 2013) [14]; as the fourth, we have used an updated model developed in this study. Good agreement was found between measurements and predictions from all four models for all major and most typical intermediate species with and without CO2 addition in low-pressure flat flame experiments. However, none of the models was able to reliably predict high-pressure flame speeds. Although the updated model improved the prediction of flame speeds for lean mixtures, errors remained for rich conditions at elevated pressure, likely due to uncertainty in the rates of CH3+H(+M)=CH4(+M) and the branching and termination reaction pair of CH3+HO2=CH3O+OH and CH3+HO2=CH4+O2. CO2 addition considerably decreased the flame speed. Kinetic comparisons between inert and chemically active CO2 in DME flames showed that CO2 addition affects rich and lean DME flame kinetics differently. For lean flames, both the inert third-body effect and the kinetic effect of CO2 reduce H-atom production. However, for rich flames, the inert third-body effect increases H-atom production via HCO(+M)=H+CO(+M) and suppression of the kinetic effect of CO2 by shifting the equilibrium of CO+OH=CO2+H.
KW - Carbon dioxide
KW - Combustion intermediates
KW - Dimethyl ether
KW - Flame speed
KW - High pressure
KW - Kinetic models
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U2 - 10.1016/j.combustflame.2013.06.032
DO - 10.1016/j.combustflame.2013.06.032
M3 - Article
AN - SCOPUS:84885293558
SN - 0010-2180
VL - 160
SP - 2654
EP - 2668
JO - Combustion and Flame
JF - Combustion and Flame
IS - 12
ER -