Abstract:Effects of lightning‐induced generation of high‐frequency and microwave radiation are of great interest for studying fundamental physics of lightning and its applications for monitoring of the thunderstorm activity and protection of equipment against electromagnetic interference. Ultrawideband electromagnetic pulses (UWB EMPs) of spark discharges about 1 m long were detected in a frequency band of up to 10 GHz in laboratory experiments using a cloud of water droplets charged up to the electric potential exceed… Show more
“…It is shown experimentally that at some phases of long electric spark development a radio-frequency emission is generated in a band of at least up to 1.4 GHz. The obtained results match with both the published natural data on radio-frequency emission of lightning [4] and the theoretical calculations [3] and measured parameters of RF emission of long streamers [6].…”
supporting
confidence: 87%
“…In [3][4][5] the RF emission of real thunderstorm clouds and lightning discharges was studied. In [6] it was found that from discharges in a charged aerosol structure (simulating a thunderstorm cell) a RF emission is generated with a frequency of up to 10 GHz.…”
On the created stand, in laboratory conditions, various phases of discharge development characteristic of lightning were simulated using an electric spark in a long air gap. With the help of special radio equipment, the radio emission of a long electric spark was investigated. It is found that at the stages of development of a spark discharge, radio emission is recorded in a long interval up to at least a frequency of 1.4 GHz. Data on radio emission in this range are of great practical importance for such areas as radio communication (during thunderstorm activity), radar, lightning direction finding. Keywords: Long electric spark, lightning discharge, radio emission, streamer discharge, lead discharge, radio communication.
“…It is shown experimentally that at some phases of long electric spark development a radio-frequency emission is generated in a band of at least up to 1.4 GHz. The obtained results match with both the published natural data on radio-frequency emission of lightning [4] and the theoretical calculations [3] and measured parameters of RF emission of long streamers [6].…”
supporting
confidence: 87%
“…In [3][4][5] the RF emission of real thunderstorm clouds and lightning discharges was studied. In [6] it was found that from discharges in a charged aerosol structure (simulating a thunderstorm cell) a RF emission is generated with a frequency of up to 10 GHz.…”
On the created stand, in laboratory conditions, various phases of discharge development characteristic of lightning were simulated using an electric spark in a long air gap. With the help of special radio equipment, the radio emission of a long electric spark was investigated. It is found that at the stages of development of a spark discharge, radio emission is recorded in a long interval up to at least a frequency of 1.4 GHz. Data on radio emission in this range are of great practical importance for such areas as radio communication (during thunderstorm activity), radar, lightning direction finding. Keywords: Long electric spark, lightning discharge, radio emission, streamer discharge, lead discharge, radio communication.
“…Both of these electromagnetic radiation formation mechanisms correlate to the characteristic frequency ranges of the wavelet spectrums of signals, and are guided on model rods and long elements of the neighboring flash of the streamer corona; these develop from another model element belonging to group II and group III, containing large force-strength factors of the electric field. Electromagnetic radiation with frequencies exceeding 1 GHz during streamer flashes in the electric field of a cloud charged with water drops was registered in [28] as well.…”
Section: Analysis Of Results and Discussionmentioning
The results of a physical simulation using negatively charged artificial thunderstorm cells to test the spectrum of possible electromagnetic effects of upward streamer discharges on the model elements of transmission line monitoring systems (sensor or antennas) are presented. Rod and elongated model elements with different electric field amplification coefficients are investigated. A generalization is made about the parameters of upward streamer current impulse and its electromagnetic effect on both kinds of model elements. A wavelet analysis of the upward streamer corona current impulse and of the signal simultaneously induced in the neighboring model element is conducted. A generalization of the spectral characteristics of the upward streamer current and of the signals induced by the electromagnetic radiation of the nearby impulse streamer corona on model elements is made. The reasons for super-high and ultra-high frequency ranges in the wavelet spectrum of the induced electromagnetic effect are discussed. The characteristic spectral ranges of the possible electromagnetic effect of upward streamer flash on the elements of transmission line monitoring systems are considered.
“…To measure pulsed electric and magnetic fields in the line directly, strip-line IPPL probes [25] and inductive TPMP probes with the rise time of the pulse characteristic being not more than 35 ps, respectively, were used. An assembly of such probes was used, e.g., to detect the shape of subnanosecond pulses generated by long spark discharges [26]. To detect the shape of an EMP after it passed through the plasma-filled line, the low-inductance dummy load with wideband attenuators was used.…”
A large-scale coaxial line filled with the plasma of RF discharge has been developed for laboratory modeling of the effects of the interaction of ultrashort electromagnetic pulses (EMPs) with the atmosphere and the ionosphere in the KROT facility. The oversized coaxial line ensures pulse transmission through an ionized medium in the TEM mode, which corresponds to the polarization of the transverse electromagnetic wave in free space, and in uniform isotropic plasma. The coaxial line has a length of 10 m and a diameter of 140 cm. The processes of propagation of the nanosecond and subnanosecond pulses in this line, in vacuum and with plasma, have been simulated numerically.
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