TY - JOUR
T1 - Microwave-plasma-coupled re-ignition of methane-and-oxygen mixture under auto-ignition temperature
AU - Rao, Xing
AU - Hammack, Stephen
AU - Carter, Campbell
AU - Grotjohn, Timothy
AU - Asmussen, Jes
AU - Lee, Tonghun
N1 - Funding Information:
Manuscript received February 25, 2011; revised May 24, 2011; accepted June 16, 2011. Date of publication August 4, 2011; date of current version December 14, 2011. This work was supported by the Air Force Office of Scientific Research under Award FA9550-09-1-0282 and Award FA9550-10-1-0556 with Dr. J. Tishkoff as Technical Monitor.
PY - 2011/12
Y1 - 2011/12
N2 - The re-ignition phenomenon is observed when fuel/oxidizer is re-introduced into an atmospheric-pressure plasma discharge generated by cutting off the gas flow in a re-entrant microwave-plasma applicator system used for plasma-assisted ignition and combustion research works. Results indicate that, for re-ignition to occur, the electric field must be strong enough to fully establish a weakly ionized and self-sustained plasma discharge, and with elevated radical concentrations. The re-ignition was possible at gas flow speeds higher than typical flame propagation rates, and temperature measurements (thermocouple and N 2 emission) reveal that re-ignition occurs under auto-ignition temperatures. The high-speed imaging of the flame propagation shows that it is a two step process of initiating a fast pyrolysis flame, which, in turn, stabilizes and starts the direct coupling process of the plasma energy into the flame for full re-ignition to occur.
AB - The re-ignition phenomenon is observed when fuel/oxidizer is re-introduced into an atmospheric-pressure plasma discharge generated by cutting off the gas flow in a re-entrant microwave-plasma applicator system used for plasma-assisted ignition and combustion research works. Results indicate that, for re-ignition to occur, the electric field must be strong enough to fully establish a weakly ionized and self-sustained plasma discharge, and with elevated radical concentrations. The re-ignition was possible at gas flow speeds higher than typical flame propagation rates, and temperature measurements (thermocouple and N 2 emission) reveal that re-ignition occurs under auto-ignition temperatures. The high-speed imaging of the flame propagation shows that it is a two step process of initiating a fast pyrolysis flame, which, in turn, stabilizes and starts the direct coupling process of the plasma energy into the flame for full re-ignition to occur.
KW - Auto-ignition temperature
KW - laser induced fluorescence
KW - plasma assisted combustion
KW - re-ignition
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U2 - 10.1109/TPS.2011.2161597
DO - 10.1109/TPS.2011.2161597
M3 - Article
AN - SCOPUS:83855160906
SN - 0093-3813
VL - 39
SP - 3307
EP - 3313
JO - IEEE Transactions on Plasma Science
JF - IEEE Transactions on Plasma Science
IS - 12 PART 1
M1 - 5971799
ER -