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Radar Reflectivity and Altitude Distributions of Lightning Flashes as a Function of Three Main Storm Types
Author(s) -
Mecikalski Retha M.,
Carey Lawrence D.
Publication year - 2018
Publication title -
journal of geophysical research: atmospheres
Language(s) - English
Resource type - Journals
eISSN - 2169-8996
pISSN - 2169-897X
DOI - 10.1029/2018jd029238
Subject(s) - mesoscale meteorology , lightning (connector) , altitude (triangle) , radar , storm , meteorology , mesoscale convective system , convective storm detection , correlation coefficient , geology , atmospheric sciences , environmental science , remote sensing , physics , mathematics , geometry , statistics , telecommunications , power (physics) , quantum mechanics , computer science
In an effort to improve our knowledge on the horizontal and vertical distribution of lightning initiation and propagation, ~500 multicells (producing a total of 72,619 flashes), 27 mesoscale convective systems (producing 214,417 flashes) and 23 supercells (producing 169,861 flashes) that occurred over northern Alabama and southern Tennessee were analyzed using data from the North Alabama Lightning Mapping Array and the Multi‐Radar Multi‐Sensor suite. From this analysis, two‐dimensional (2‐D) histograms of where flashes initiated and propagated relative to radar reflectivity and altitude were created for each storm type. The peak of the distributions occurred between 8.0 and 10.0 km (−24.0 to −38.5 °C) and between 30 and 35 dB Z for flashes that initiated within multicellular storms. For flashes that initiated within mesoscale convective systems, these peaks were 8.0–9.0 km (−27.1 to −34.6 °C) and 30–35 dB Z , respectively, and for supercells, they were 10.0–12.0 km (−42.6 to −58.1 °C) and 35–40 dB Z , respectively. The 2‐D histograms for the flash propagations were slightly different than for the flash initiations and showed that flashes propagated in lower reflectivities as compared to where they initiated. The 2‐D histograms were also compared to test cases; the root‐mean‐square errors and the Pearson product moment correlation coefficient ( R ) were calculated with several of the comparisons having R values >0.7 while the root‐mean‐square errors were always ≤0.017 (≤10%), irrespective of storm type. Finally, the mean flash sizes for the multicell, mesoscale convective system, and supercell flashes were 8.3, 9.9, and 7.4 km, respectively.

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