Abstract The initial discharge stages of two flashes during the Shandong Artificially Triggering Lightning Experiment (SHATLE) are analyzed based on the synchronous data of the current and close electromagnetic field. For a lightning flash, named 0503, the wire was connected, not electrically, but via a 5 m length of nylon, with the lightning rod; while for another, named 0602, the wire was connected with the rod directly. Results show that the discharge processes of the initial stage (IS) in flash 0503 are quite different from that of the usual classical-triggered flash 0602 and altitude-triggered flashes. A large pulse with a current of about 720 A resulted from the breakdown of the 5 m air gap during flash 0503, and the corresponding electric field at 60 m from the lightning rod was 0.38 kV/m. The upward positive leaders (UPLs) propagated continuously from the tip of the rocket after this breakdown. The geometric mean (GM) of the UPL peak current was 23.0 A. Vaporization of the wire occurred during the initial continuous current (ICC) stage and the largest current pulse was about 400 A. Compared with triggered flash 0503, the discharge processes of IS in flash 0602 were simple, only two large pulses similar to each other occurred before dart leader/return stroke sequences. The peak current of the first pulse was 2.1 kA and its corresponding electric field and magnetic field at a distance of 60 m from the lightning rod were 0.98 kV/m and 7.03 μT, respectively. During the second pulse, the wire disintegrated. The current decreased to the background level at the moment of the wire disintegration. The current of the second pulse in triggered flash 0602 was 2.8 kA, and the corresponding electric field and magnetic field at 60 m from the lightning rod were 1.22 kV/m and 9.01 μT, respectively.
[1]
K. B. McEachron,et al.
Lightning to the Empire State Building
,
1939,
Transactions of the American Institute of Electrical Engineers.
[2]
Vladimir A. Rakov,et al.
A review of ten years of triggered-lightning experiments at Camp Blanding, Florida
,
2005
.
[3]
M. Uman,et al.
The Lightning Discharge
,
1987
.
[4]
Xiushu Qie,et al.
Magnetic field measuring system and current retrieval in artificially triggering lightning experiment
,
2008
.
[5]
Vladimir A. Rakov,et al.
Cutoff and reestablishment of current in rocket-triggered lightning
,
2003
.
[6]
V. Rakov,et al.
Lightning: Physics and Effects
,
2007
.
[7]
Vladimir A. Rakov,et al.
Characterization of the initial stage of negative rocket‐triggered lightning
,
1999
.
[8]
E. A. Lewis,et al.
Triggered lightning strokes at very close range
,
1967
.
[9]
Yunjun Zhou,et al.
Characteristics of triggered lightning during Shandong artificial triggering lightning experiment (SHATLE)
,
2009
.
[10]
Qilin Zhang,et al.
Characteristics and simulation of lightning current waveforms during one artificially triggered lightning
,
2009
.
[11]
Jing Yang,et al.
Artificially triggered lightning and its characteristic discharge parameters in two severe thunderstorms
,
2006
.
[12]
Vladimir A. Rakov,et al.
Leader properties determined with triggered lightning techniques
,
1998
.