2022
DOI: 10.1016/j.combustflame.2022.112424
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Energy deposition and plasma propulsion during the time window of microwave-assisted CH4-O2 spark ignition with Ar/N2/CO2 dilution

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Cited by 6 publications
(1 citation statement)
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“…It was apparent that the MW power mainly governed the critical C NH3,i , affecting an almost linear increase of the critical C NH3,i with P MW , whereas the total flow rate was secondary, demonstrating relatively small negative impact on the critical C NH3,i for a given P MW (figure 4). MW discharge has been known to operate in a relatively low electric field, having difficulties in igniting by itself, and thus it requires an external source for seed elections to breakdown a gaseous media [42][43][44][45]. As ammonia was added, not only some portion of the total electron energy was transferred to NH 3 but also the excited states of Ar lost their energy due to the collisions with NH 3 , resulted in less ionization of Ar [38].…”
Section: Addition Of Ammoniamentioning
confidence: 99%
“…It was apparent that the MW power mainly governed the critical C NH3,i , affecting an almost linear increase of the critical C NH3,i with P MW , whereas the total flow rate was secondary, demonstrating relatively small negative impact on the critical C NH3,i for a given P MW (figure 4). MW discharge has been known to operate in a relatively low electric field, having difficulties in igniting by itself, and thus it requires an external source for seed elections to breakdown a gaseous media [42][43][44][45]. As ammonia was added, not only some portion of the total electron energy was transferred to NH 3 but also the excited states of Ar lost their energy due to the collisions with NH 3 , resulted in less ionization of Ar [38].…”
Section: Addition Of Ammoniamentioning
confidence: 99%