TY - JOUR
T1 - Quantitative research on cellular instabilities of premixed C1–C3 alkane–air mixtures using spherically expanding flames
AU - Zuo, Zinong
AU - Hu, Bo
AU - Bao, Xiuchao
AU - Zhang, Shibo
AU - Kong, Lingan
AU - Deng, Lang
AU - Xu, Yibo
AU - Zhu, Zhennan
AU - Pan, Suozhu
PY - 2022/2
Y1 - 2022/2
N2 - The cellular instabilities of premixed C1–C3 alkane–air mixtures were investigated at an initial temperature of 400 K and different initial pressures (0.25–1.5 MPa). Flame propagation images were recorded using high-speed Schlieren photography techniques. Cellular instabilities were analyzed using both qualitative and quantitative methods. The results showed that with an increase in the initial pressure, the flame instabilities of these three alkane–air mixtures increased as a result of the enhanced hydrodynamic instability. For a given initial pressure and with an increasing equivalence ratio, the thermal-diffusive instability was the main influencing factor on the flame instability of methane when Φ ≤ 1.0, whereas it was the result of hydrodynamic and thermal-diffusive instability when Φ > 1.0. The flame instability of ethane and propane was caused by the enhanced hydrodynamic and thermal-diffusive instability when Φ ≤ 1.0, whereas it was determined by diffusion-thermal instability when Φ > 1.0. Under the conditions with the strongest cellular instability, the cellular instability of these three alkane–air mixtures tended to increase with an increasing number of carbon atoms in the fuel.
AB - The cellular instabilities of premixed C1–C3 alkane–air mixtures were investigated at an initial temperature of 400 K and different initial pressures (0.25–1.5 MPa). Flame propagation images were recorded using high-speed Schlieren photography techniques. Cellular instabilities were analyzed using both qualitative and quantitative methods. The results showed that with an increase in the initial pressure, the flame instabilities of these three alkane–air mixtures increased as a result of the enhanced hydrodynamic instability. For a given initial pressure and with an increasing equivalence ratio, the thermal-diffusive instability was the main influencing factor on the flame instability of methane when Φ ≤ 1.0, whereas it was the result of hydrodynamic and thermal-diffusive instability when Φ > 1.0. The flame instability of ethane and propane was caused by the enhanced hydrodynamic and thermal-diffusive instability when Φ ≤ 1.0, whereas it was determined by diffusion-thermal instability when Φ > 1.0. Under the conditions with the strongest cellular instability, the cellular instability of these three alkane–air mixtures tended to increase with an increasing number of carbon atoms in the fuel.
KW - Alkane
KW - Average cell size
KW - Cellular instability
KW - Constant volume combustion vessel (CVCV)
KW - Quantitative research
UR - http://www.scopus.com/inward/record.url?scp=85117763455&partnerID=8YFLogxK
UR - https://www.sciencedirect.com/science/article/pii/S0378382021003568?via%3Dihub
U2 - 10.1016/j.fuproc.2021.107075
DO - 10.1016/j.fuproc.2021.107075
M3 - Article
AN - SCOPUS:85117763455
SN - 0378-3820
VL - 226
JO - Fuel Processing Technology
JF - Fuel Processing Technology
M1 - 107075
ER -