How pulse energy affects ignition efficiency of DBD plasma-assisted combustion

被引:3
作者
Patel, Ravi [1 ,2 ]
Peelen, Rik [1 ]
van Oijen, Jeroen [2 ]
Dam, Nico [2 ]
Nijdam, Sander [1 ]
机构
[1] Eindhoven Univ Technol, Dept Appl Phys, POB 513, NL-5600 MB Eindhoven, Netherlands
[2] Eindhoven Univ Technol, Dept Mech Engn, POB 513, NL-5600 MB Eindhoven, Netherlands
关键词
plasma-assisted combustion; pulsed DBD plasma; DBD equivalent circuit model; optical emission spectroscopy; minimum ignition energy; DIELECTRIC-BARRIER DISCHARGES; AIR FLOWS; NANOSECOND; MIXTURES; FLAMES;
D O I
10.1088/1361-6463/acf942
中图分类号
O59 [应用物理学];
学科分类号
摘要
This work aims to find how coupled energy per pulse influences the ability of a pulsed dielectric barrier discharge (DBD) plasma to ignite fuel-lean methane-air flow. For that, experiments are performed on a custom-built DBD flow reactor with a variable dielectric thickness and the discharge is operated by bursts of 10 ns duration pulses at 3 kHz repetition rate. With an increase in dielectric thickness, we observe that the coupled energy per pulse decreases even though applied voltage conditions are similar and so more pulses are required to ignite the lean mixture. Interestingly, we observe a significant increase in the minimum ignition energy (MIE) with an increase in the thickness beyond 3 mm. Moreover, the ignition kernel growth rate is much slower in the thicker dielectric cases even though total energy coupling per burst is similar. This phenomenon is investigated further by evaluating plasma parameters using electrical and optical diagnostics. Effective dielectric capacitance, discharge current, and voltage drop across the gas gap are derived from an equivalent circuit analysis, whereas plasma gas temperature and effective reduced electric field ( E/N ) are estimated from optical emission spectroscopy. From these analyses, we conclude that a thicker dielectric limits the discharge current and so the plasma filament temperature. For more than 3 mm thick dielectric cases, the filament heating per pulse is too low to achieve strong enough plasma pulse-to-pulse coupling which eventually leads to higher MIE and slower ignition kernel growth rate or the inability to ignite at all.
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页数:15
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