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Characteristics of Electric Currents in Upward Lightning Flashes From a Windmill and its Lightning Protection Tower in Japan, 2005–2016
Author(s) -
Wang Xiankang,
Wang Daohong,
He Junjia,
Takagi Nobuyuki
Publication year - 2021
Publication title -
journal of geophysical research: atmospheres
Language(s) - English
Resource type - Journals
eISSN - 2169-8996
pISSN - 2169-897X
DOI - 10.1029/2020jd034346
Subject(s) - lightning (connector) , tower , waveform , current (fluid) , meteorology , thunderstorm , physics , environmental science , peak current , electrical engineering , atmospheric sciences , voltage , engineering , power (physics) , structural engineering , quantum mechanics , thermodynamics , electrode , electrochemistry
We examine the lightning current of 81 upward lightning (UL) initiated from a windmill and its lightning protection tower in Japan under winter thunderstorms from 2005 to 2016. Among 81 UL, the negative, positive, and bipolar lightning account for 64%, 12%, and 24%, respectively. After checking the current waveforms during the initial stage (IS) of negative UL, we found that self‐initiated negative UL have larger peak value and shorter rise time compared to other‐triggered ones, although two types of negative UL show no significant difference in charge transfer and duration. Among 18 self‐initiated negative UL, half of them are initiated from the windmill. On the other hand, only two of 27 other‐triggered negative UL are from the windmill and both of them have smaller current peak value, shorter duration, and smaller charge transfer. According to whether or not the IS current waveforms exhibit pulsation, we have classified UL into type S (smooth), SP (transition from smooth to pulsation), and P (pulsation). We found that the rate of slow current rise for most type P UL is larger than 0.1 kA/ms, whereas for all type S UL the rate is smaller than 0.01 kA/ms. The type SP UL shows a slow current rise rate ranging from 0.01 to 0.1 kA/ms. We found that the current pulsation of type P UL corresponds to the stepwise propagation of a positive leader. Based on these results, we have discussed the effect of the lightning protection tower and the stepwise propagation of positive leaders.