1993
DOI: 10.1109/27.221123
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Electron current to a cylindrical probe in a moving high pressure plasma

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Cited by 15 publications
(6 citation statements)
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“…An explanation of this disagreement between ICSPA and PPA can be found in Franke et al 51 who observed that the weakness of the correspondence between ICSPA and PPA occurs in configurations that convert high gas flow in the vicinity of the spark plug electrode gap at ignition – to high turbulence regime in proximity of peak pressure, and considered this turbulence as reason of the weak agreement between ICSPA and PPA. Actually, in the IC measurement, the spark plug tip basically works as a Langmuir probe, as shown in Strandh et al 27 Thus the conclusion of Franke et al 51 is consistent with the observation of Dawe et al 56 who found that the electron current flowing in a positively biased cylindrical probe immersed in a moving plasma is influenced by flow velocity. This proves that IC signal variability cannot be attributed to noise, but to other variables that were not considered, such as local gas flow velocity.…”
Section: Discussionsupporting
confidence: 71%
“…An explanation of this disagreement between ICSPA and PPA can be found in Franke et al 51 who observed that the weakness of the correspondence between ICSPA and PPA occurs in configurations that convert high gas flow in the vicinity of the spark plug electrode gap at ignition – to high turbulence regime in proximity of peak pressure, and considered this turbulence as reason of the weak agreement between ICSPA and PPA. Actually, in the IC measurement, the spark plug tip basically works as a Langmuir probe, as shown in Strandh et al 27 Thus the conclusion of Franke et al 51 is consistent with the observation of Dawe et al 56 who found that the electron current flowing in a positively biased cylindrical probe immersed in a moving plasma is influenced by flow velocity. This proves that IC signal variability cannot be attributed to noise, but to other variables that were not considered, such as local gas flow velocity.…”
Section: Discussionsupporting
confidence: 71%
“…Since the flame is a quasineutral thermal plasma, the number concentration of positive ions must equal the number concentration of negative ions plus electrons (n + = n − + n e ) at any location in the flame [25,26]. On this basis we can readily calculate the number concentration of negative ions, which is of similar concentration with positive ions, due to the small concentration of electrons compared with that of positive ions as measured by the Langmuir double probe.…”
Section: Methodsmentioning
confidence: 98%
“…This region is rarely considered in the literature for the purpose of the electron temperature determination, although some work has been published in the frame of Orbital Motion Limit theories [87]. Also, in [80,81] this region is used because it provides high currents in their relatively low pressure (and low ionization) regimes.…”
Section: ) Electron and Ion Velocities Have A Maxwellian Distributionmentioning
confidence: 99%
“…To the author's knowledge, the works dealing with these high values are only Clements and Smy's paper of 1972 [113] and Holmes et al [105]. Also, Dawe et al [81], while stating the validity of the "sheath convection mode" (attributed to Smy [84] for regimes from 10 20 m -3 up to 10 29 m -3 (evidently a print error! ), limits his experimental analysis to flames similar to those discussed by Clements and Smy [79,91,111,114,115].…”
Section: Introductionmentioning
confidence: 98%
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