Transient current pulses in rocket-extended wires used to trigger lightning

被引:22
作者
Biagi, C. J. [1 ]
Uman, M. A. [1 ]
Hill, J. D. [1 ]
Rakov, V. A. [1 ]
Jordan, D. M. [1 ]
机构
[1] Univ Florida, Dept Elect & Comp Engn, Gainesville, FL 32611 USA
基金
美国国家科学基金会;
关键词
MODEL; REPRESENTATION; LEADERS;
D O I
10.1029/2011JD016161
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
We analyze current, electric field, and optical signatures of the sudden electrical breakdown processes (precursors) that occur at the top of the upward extending, grounded, Kevlar-covered copper wires used to artificially trigger lightning. For one launch, before the sustained upward positive leader initiated, we estimate that up to 10,000 precursors occurred (one every few hundred microseconds) with peak currents from 1 to more than 100 A. Luminosity at the wire tip was observed for 339 of 410 precursors examined in detail and, in seven cases, discharge channels developed to lengths of 3 to 8 m over times of several hundred microseconds. The measured propagation speeds of current pulses on the triggering wires were less than the speed of light, and decreased from about 2.8 x 10(8) m s (-1) to about 2.3 x 10(8) m s (-1) with increasing wire-top heights from about 80 m to about 340 m. The triggering wire and its grounding system are modeled as uniform transmission lines with model predictions that are consistent with the measured wire-base precursor current signatures. The modeling shows that (1) the characteristic impedance of the triggering wire, the ratio of the propagating precursor voltage pulse to its associated current pulse, is between 600 and 800 Omega; (2) the 25 m ground rod grounding impedance for the peak precursor current is about 100 Omega, while the DC grounding resistance is 20 Omega; and (3) the current reflection coefficient at ground for peak precursor current is similar to 0.9.
引用
收藏
页数:16
相关论文
共 22 条
[1]   On the mechanism of attenuation of current waves propagating along a vertical perfectly conducting wire above ground: Application to lightning [J].
Baba, Y ;
Rakov, VA .
IEEE TRANSACTIONS ON ELECTROMAGNETIC COMPATIBILITY, 2005, 47 (03) :521-532
[2]   On the transmission line model for lightning return stroke representation [J].
Baba, Y ;
Rakov, VA .
GEOPHYSICAL RESEARCH LETTERS, 2003, 30 (24) :ASC13-1
[3]  
BAZELYAN EM, 1978, PHYS ENG FDN LIGHTNI
[4]   Determination of the electric field intensity and space charge density versus height prior to triggered lightning [J].
Biagi, C. J. ;
Uman, M. A. ;
Gopalakrishnan, J. ;
Hill, J. D. ;
Rakov, V. A. ;
Ngin, T. ;
Jordan, D. M. .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2011, 116
[5]   High-speed video observations of rocket-and-wire initiated lightning [J].
Biagi, C. J. ;
Jordan, D. M. ;
Uman, M. A. ;
Hill, J. D. ;
Beasley, W. H. ;
Howard, J. .
GEOPHYSICAL RESEARCH LETTERS, 2009, 36
[6]   A MODEL FOR SUBSEQUENT RETURN STROKES [J].
COORAY, V .
JOURNAL OF ELECTROSTATICS, 1993, 30 :343-354
[7]   The close lightning electromagnetic environment: Dart-leader electric field change versus distance [J].
Crawford, DE ;
Rakov, VA ;
Uman, MA ;
Schnetzer, GH ;
Rambo, KJ ;
Stapleton, MV ;
Fisher, RJ .
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2001, 106 (D14) :14909-14917
[8]  
Herniter M. E, 2002, SCHEMATIC CAPTURE CA
[9]  
Horii K., 1982, Memoirs of the Faculty of Engineering, Nagoya University, V34, P77
[10]  
Jerauld J., 2007, THESIS U FLA GAINESV