Positive double-pulse streamers: how pulse-to-pulse delay influences initiation and propagation of subsequent discharges
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Li, Y.
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Xi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Eindhoven Univ Technol, Dept Appl Phys, POB 513, NL-5600 MB Eindhoven, NetherlandsXi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Li, Y.
[1
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van Veldhuizen, E. M.
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Eindhoven Univ Technol, Dept Appl Phys, POB 513, NL-5600 MB Eindhoven, NetherlandsXi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
van Veldhuizen, E. M.
[2
]
Zhang, G. J.
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Xi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R ChinaXi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Zhang, G. J.
[1
]
Ebert, U.
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Eindhoven Univ Technol, Dept Appl Phys, POB 513, NL-5600 MB Eindhoven, Netherlands
CWI, Amsterdam, NetherlandsXi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Ebert, U.
[2
,3
]
Nijdam, S.
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Eindhoven Univ Technol, Dept Appl Phys, POB 513, NL-5600 MB Eindhoven, NetherlandsXi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Nijdam, S.
[2
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[1] Xi An Jiao Tong Univ, State Key Lab Elect Insulat & Power Equipment, Xian 710049, Shaanxi, Peoples R China
Residual charges and species created by previous streamers have a great impact on the characteristics of the next discharge. This is especially pronounced in repetitively pulsed discharges, where the physical and chemical reactions during the decay phase play a very important role. We have performed double-pulse streamer experiments in artificial air and pure nitrogen with a varying pulse delay (Delta t) from 0.45 mu s to 20 ms. We have observed morphological transformations of the 2nd-pulse streamer as a function of Delta t and classified six typical stages by streamer length. The propagation distance of the 2nd-pulse streamer can be 66% longer than the 1st-pulse in 66.7 mbar nitrogen, while it is 37% longer in air under the same conditions. However, we find that the longer propagation distance of the 2nd-pulse streamer in N-2 is not caused by a higher velocity nor by fast gas heating of previous channels under our experimental conditions, but by earlier inception which gives more time to propagate during the pulse. In air, on the other hand, the streamers initiate almost at the same time in both pulses but the inception cloud of the 2nd-pulse streamer breaks up earlier. The onset of every stage occurs at smaller Delta t in air than in N-2 at the same pressure. These observations imply that different mechanisms work in N-2 and air, e.g. photoionization and attachment.