Triggering and guiding of an upward positive leader from a ground rod with an ultrashort laser pulse -: II:: Modeling

被引:21
作者
Comtois, D [1 ]
Pépin, H
Vidal, F
Rizk, FAM
Chien, CY
Johnston, TW
Kieffer, JC
La Fontaine, B
Martin, F
Potvin, C
Couture, P
Mercure, HP
Bondiou-Clergerie, A
Lalande, P
Gallimberti, I
机构
[1] INRS Energie Mat & Telecommun, Varennes, PQ J3X 1S2, Canada
[2] Inst Rech Hydro Quebec, Varennes, PQ J3X 1S1, Canada
[3] Off Natl Etud & Rech Aerosp, F-92322 Chatillon, France
[4] Univ Padua, Dept Elect Engn, I-35100 Padua, Italy
基金
加拿大自然科学与工程研究理事会;
关键词
breakdown; discharge; laser; leader; lightning; ultrashort;
D O I
10.1109/TPS.2003.811649
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
We have used the Bondio-Gallimberti model of positive leader propagation to simulate laboratory experiments of laser triggering and guiding of upward leaders initiated from a ground rod. The model proves to be capable of reproducing all the important features of laser-guided leader propagation that have been ob served experimentally. The leader guiding effect of the laser-created plasma channel is taken into account in the model by adjusting the value of the charge per unit length of the leader, which has been measured in the laboratory to be lower for a laser-guided leader than for an ordinary one. The charge per unit length of the leader is related in the model to the critical temperature at which the air in the transition region at the leader tip must be heated to be conductive enough to become a new leader portion. For an ordinary leader, this critical temperature is 1500 K; at which the electrons all detach from the negative ions in the leader corona, increasing the air conductivity. We give the interpretation that in the case of the laser-guided leaders, because of the relatively high density of negative ions per unit length in the laser-ionized channel, the right conditions of conductivity can be met in the transition region without the electrons being all detached from the ions, allowing a reduction of the critical temperature and of the charge per unit length.
引用
收藏
页码:387 / 395
页数:9
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