Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields
The authors present an analysis of different charge transfer modes during upward negative flashes. The analysis includes a total number of 94 pulses that occurred during two upward negative flashes recorded at the Säntis Tower. The pulses included 59 mixed-mode (MM) initial continuous current (ICC)...
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doaj-8342d28663294a8eb632c6ec021da7422021-04-02T15:23:41ZengWileyHigh Voltage2397-72642019-05-0110.1049/hve.2019.0017HVE.2019.0017Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fieldsLixia He0Mohammad Azadifar1Quanxin Li2Marcos Rubinstein3Vladimir A. Rakov4Vladimir A. Rakov5Arturo Mediano6Davide Pavanello7Farhad Rachidi8Electromagnetic Compatibility Laboratory, Swiss Federal Institute of Technology (EPFL)Electromagnetic Compatibility Laboratory, Swiss Federal Institute of Technology (EPFL)Electromagnetic Compatibility Laboratory, Swiss Federal Institute of Technology (EPFL)University of Applied Sciences of Western Switzerland (HES-SO)Department of Electrical and Computer Engineering, University of FloridaDepartment of Electrical and Computer Engineering, University of FloridaDepartment Electronics and Communication Engineering, University of ZaragozaInstitute of Sustainable Energy, University of Applied Sciences of Western Switzerland (HES-SO)Electromagnetic Compatibility Laboratory, Swiss Federal Institute of Technology (EPFL)The authors present an analysis of different charge transfer modes during upward negative flashes. The analysis includes a total number of 94 pulses that occurred during two upward negative flashes recorded at the Säntis Tower. The pulses included 59 mixed-mode (MM) initial continuous current (ICC) pulses, 17 M-component-type ICC (M-ICC) pulses, 8 return-stroke pulses, and 10 classical M-component (MC) pulses. It is found that the initial stage of the flash is responsible for the largest share of the total charge transferred to the ground. Simulation results for the electric fields associated with the considered charge transfer modes are presented and discussed. Return stroke (RS) and MM pulses were simulated adopting the MTLE model, while MCs and M-ICC pulses were simulated using the guided wave model of Rakov et al. The simulated results are shown to be in good agreement with simultaneous records of electric fields measured at a distance of 15 km from the Säntis Tower. The inferred velocities for MCs and M-ICC pulses range from 2.0 × 10^7 to 9.0 × 10^7 m/s, and the corresponding junction point heights range from 1.0 to 2.0 km. The inferred pulse velocities for RSs and MM pulses range from 1.3 × 10^8 to 1.65 × 10^8 m/s. The inferred current attenuation constants of the MTLE model obtained in this study range from 0.3 to 0.8 km, lower than the value of 2 km previously suggested for RSs in downward flashes. The obtained results support the assumption that the mode of charge transfer to the ground giving rise to MM pulses is similar to that of RSs. The results are also in support of the generally assumed similarity between M-ICC pulses and classical MCs.https://digital-library.theiet.org/content/journals/10.1049/hve.2019.0017poles and towerslightninginferred pulse velocitiesmm pulsesinferred current attenuation constantsmtle modeldownward flashesupward negative flashessäntis towermixed-mode initial continuous current pulsesm-component-type icc pulsestotal chargeelectric fieldsreturn strokecharge transfer modesreturn-stroke pulsesclassical m-component pulsesguided wave modelsize 0.3 km to 0.8 kmaltitude 1.0 km to 2.0 kmdistance 15.0 km |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Lixia He Mohammad Azadifar Quanxin Li Marcos Rubinstein Vladimir A. Rakov Vladimir A. Rakov Arturo Mediano Davide Pavanello Farhad Rachidi |
spellingShingle |
Lixia He Mohammad Azadifar Quanxin Li Marcos Rubinstein Vladimir A. Rakov Vladimir A. Rakov Arturo Mediano Davide Pavanello Farhad Rachidi Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields High Voltage poles and towers lightning inferred pulse velocities mm pulses inferred current attenuation constants mtle model downward flashes upward negative flashes säntis tower mixed-mode initial continuous current pulses m-component-type icc pulses total charge electric fields return stroke charge transfer modes return-stroke pulses classical m-component pulses guided wave model size 0.3 km to 0.8 km altitude 1.0 km to 2.0 km distance 15.0 km |
author_facet |
Lixia He Mohammad Azadifar Quanxin Li Marcos Rubinstein Vladimir A. Rakov Vladimir A. Rakov Arturo Mediano Davide Pavanello Farhad Rachidi |
author_sort |
Lixia He |
title |
Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
title_short |
Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
title_full |
Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
title_fullStr |
Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
title_full_unstemmed |
Characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
title_sort |
characteristics of different charge transfer modes in upward flashes inferred from simultaneously measured currents and fields |
publisher |
Wiley |
series |
High Voltage |
issn |
2397-7264 |
publishDate |
2019-05-01 |
description |
The authors present an analysis of different charge transfer modes during upward negative flashes. The analysis includes a total number of 94 pulses that occurred during two upward negative flashes recorded at the Säntis Tower. The pulses included 59 mixed-mode (MM) initial continuous current (ICC) pulses, 17 M-component-type ICC (M-ICC) pulses, 8 return-stroke pulses, and 10 classical M-component (MC) pulses. It is found that the initial stage of the flash is responsible for the largest share of the total charge transferred to the ground. Simulation results for the electric fields associated with the considered charge transfer modes are presented and discussed. Return stroke (RS) and MM pulses were simulated adopting the MTLE model, while MCs and M-ICC pulses were simulated using the guided wave model of Rakov et al. The simulated results are shown to be in good agreement with simultaneous records of electric fields measured at a distance of 15 km from the Säntis Tower. The inferred velocities for MCs and M-ICC pulses range from 2.0 × 10^7 to 9.0 × 10^7 m/s, and the corresponding junction point heights range from 1.0 to 2.0 km. The inferred pulse velocities for RSs and MM pulses range from 1.3 × 10^8 to 1.65 × 10^8 m/s. The inferred current attenuation constants of the MTLE model obtained in this study range from 0.3 to 0.8 km, lower than the value of 2 km previously suggested for RSs in downward flashes. The obtained results support the assumption that the mode of charge transfer to the ground giving rise to MM pulses is similar to that of RSs. The results are also in support of the generally assumed similarity between M-ICC pulses and classical MCs. |
topic |
poles and towers lightning inferred pulse velocities mm pulses inferred current attenuation constants mtle model downward flashes upward negative flashes säntis tower mixed-mode initial continuous current pulses m-component-type icc pulses total charge electric fields return stroke charge transfer modes return-stroke pulses classical m-component pulses guided wave model size 0.3 km to 0.8 km altitude 1.0 km to 2.0 km distance 15.0 km |
url |
https://digital-library.theiet.org/content/journals/10.1049/hve.2019.0017 |
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