Loading…

Electrical structure in thunderstorm convective regions. Part 3: Synthesis

In this paper, results from nearly 50 electric field soundings through convective regions of mesoscale convective systems (MCSs), isolated supercells, and isolated New Mexican mountain storms are compared and synthesized. These three types of thunderstorm convection are found to have a common, basic...

Full description

Saved in:
Bibliographic Details
Published in:Journal of Geophysical Research, Washington, DC Washington, DC, 1998-01, Vol.103 (D12), p.14097-14108
Main Authors: Stolzenburg, Maribeth, Rust, WDavid, Marshall, Thomas C
Format: Article
Language:English
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by
cites
container_end_page 14108
container_issue D12
container_start_page 14097
container_title Journal of Geophysical Research, Washington, DC
container_volume 103
creator Stolzenburg, Maribeth
Rust, WDavid
Marshall, Thomas C
description In this paper, results from nearly 50 electric field soundings through convective regions of mesoscale convective systems (MCSs), isolated supercells, and isolated New Mexican mountain storms are compared and synthesized. These three types of thunderstorm convection are found to have a common, basic electrical structure. Within convective updrafts the basic charge structure has four charge regions, alternating in polarity, and the lowest is positive. Outside updrafts of convection there are typically at least six charge regions, alternating in polarity, and the lowest is again positive. Among the three storm types, there are differences in the heights and temperatures at which the basic four charge regions are found in updrafts. The height (temperature) of the center of the main negative charge region averages 6.93 km (-16 degrees C) in MCS convective region updrafts, 9.12 km (-22 degrees C) in supercell updrafts, and 6.05 km (-7 degrees C) in New Mexican mountain storm updrafts. In updraft soundings through all three storm types, the center height of the main negative charge region increases with increasing average balloon ascent rate and updraft speed at a rate of about 0.3 km per 1 m s super(-) super(1) , with a correlation coefficient of 0.94. A schematic illustrates the basic four- and six-charge structure for thunderstorm convective regions, and it is offered as an improved model for thunderstorm charge structure.
format article
fullrecord <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_miscellaneous_18123824</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>18123824</sourcerecordid><originalsourceid>FETCH-proquest_miscellaneous_181238243</originalsourceid><addsrcrecordid>eNqNyrEKwjAUQNEMChbtP7zJrZK0UYurVMRJ0L2E-LSRNNG8pODf28EP8C53OROWcSHrgpfldsZyoicfk-uN5CJjp8aijsFoZYFiSDqmgGAcxC65GwaKPvSgvRtGZgaEgA_jHa3grEKEageXj4sdkqEFm96VJcx_n7Plobnuj8Ur-HdCim1vSKO1yqFP1IpalFVdyupv-AW9j0Bq</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>18123824</pqid></control><display><type>article</type><title>Electrical structure in thunderstorm convective regions. Part 3: Synthesis</title><source>Wiley-Blackwell AGU Digital Library</source><creator>Stolzenburg, Maribeth ; Rust, WDavid ; Marshall, Thomas C</creator><creatorcontrib>Stolzenburg, Maribeth ; Rust, WDavid ; Marshall, Thomas C</creatorcontrib><description>In this paper, results from nearly 50 electric field soundings through convective regions of mesoscale convective systems (MCSs), isolated supercells, and isolated New Mexican mountain storms are compared and synthesized. These three types of thunderstorm convection are found to have a common, basic electrical structure. Within convective updrafts the basic charge structure has four charge regions, alternating in polarity, and the lowest is positive. Outside updrafts of convection there are typically at least six charge regions, alternating in polarity, and the lowest is again positive. Among the three storm types, there are differences in the heights and temperatures at which the basic four charge regions are found in updrafts. The height (temperature) of the center of the main negative charge region averages 6.93 km (-16 degrees C) in MCS convective region updrafts, 9.12 km (-22 degrees C) in supercell updrafts, and 6.05 km (-7 degrees C) in New Mexican mountain storm updrafts. In updraft soundings through all three storm types, the center height of the main negative charge region increases with increasing average balloon ascent rate and updraft speed at a rate of about 0.3 km per 1 m s super(-) super(1) , with a correlation coefficient of 0.94. A schematic illustrates the basic four- and six-charge structure for thunderstorm convective regions, and it is offered as an improved model for thunderstorm charge structure.</description><identifier>ISSN: 0148-0227</identifier><language>eng</language><ispartof>Journal of Geophysical Research, Washington, DC, 1998-01, Vol.103 (D12), p.14097-14108</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784</link.rule.ids></links><search><creatorcontrib>Stolzenburg, Maribeth</creatorcontrib><creatorcontrib>Rust, WDavid</creatorcontrib><creatorcontrib>Marshall, Thomas C</creatorcontrib><title>Electrical structure in thunderstorm convective regions. Part 3: Synthesis</title><title>Journal of Geophysical Research, Washington, DC</title><description>In this paper, results from nearly 50 electric field soundings through convective regions of mesoscale convective systems (MCSs), isolated supercells, and isolated New Mexican mountain storms are compared and synthesized. These three types of thunderstorm convection are found to have a common, basic electrical structure. Within convective updrafts the basic charge structure has four charge regions, alternating in polarity, and the lowest is positive. Outside updrafts of convection there are typically at least six charge regions, alternating in polarity, and the lowest is again positive. Among the three storm types, there are differences in the heights and temperatures at which the basic four charge regions are found in updrafts. The height (temperature) of the center of the main negative charge region averages 6.93 km (-16 degrees C) in MCS convective region updrafts, 9.12 km (-22 degrees C) in supercell updrafts, and 6.05 km (-7 degrees C) in New Mexican mountain storm updrafts. In updraft soundings through all three storm types, the center height of the main negative charge region increases with increasing average balloon ascent rate and updraft speed at a rate of about 0.3 km per 1 m s super(-) super(1) , with a correlation coefficient of 0.94. A schematic illustrates the basic four- and six-charge structure for thunderstorm convective regions, and it is offered as an improved model for thunderstorm charge structure.</description><issn>0148-0227</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1998</creationdate><recordtype>article</recordtype><recordid>eNqNyrEKwjAUQNEMChbtP7zJrZK0UYurVMRJ0L2E-LSRNNG8pODf28EP8C53OROWcSHrgpfldsZyoicfk-uN5CJjp8aijsFoZYFiSDqmgGAcxC65GwaKPvSgvRtGZgaEgA_jHa3grEKEageXj4sdkqEFm96VJcx_n7Plobnuj8Ur-HdCim1vSKO1yqFP1IpalFVdyupv-AW9j0Bq</recordid><startdate>19980101</startdate><enddate>19980101</enddate><creator>Stolzenburg, Maribeth</creator><creator>Rust, WDavid</creator><creator>Marshall, Thomas C</creator><scope>7TG</scope><scope>KL.</scope></search><sort><creationdate>19980101</creationdate><title>Electrical structure in thunderstorm convective regions. Part 3: Synthesis</title><author>Stolzenburg, Maribeth ; Rust, WDavid ; Marshall, Thomas C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_181238243</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1998</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Stolzenburg, Maribeth</creatorcontrib><creatorcontrib>Rust, WDavid</creatorcontrib><creatorcontrib>Marshall, Thomas C</creatorcontrib><collection>Meteorological &amp; Geoastrophysical Abstracts</collection><collection>Meteorological &amp; Geoastrophysical Abstracts - Academic</collection><jtitle>Journal of Geophysical Research, Washington, DC</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Stolzenburg, Maribeth</au><au>Rust, WDavid</au><au>Marshall, Thomas C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electrical structure in thunderstorm convective regions. Part 3: Synthesis</atitle><jtitle>Journal of Geophysical Research, Washington, DC</jtitle><date>1998-01-01</date><risdate>1998</risdate><volume>103</volume><issue>D12</issue><spage>14097</spage><epage>14108</epage><pages>14097-14108</pages><issn>0148-0227</issn><abstract>In this paper, results from nearly 50 electric field soundings through convective regions of mesoscale convective systems (MCSs), isolated supercells, and isolated New Mexican mountain storms are compared and synthesized. These three types of thunderstorm convection are found to have a common, basic electrical structure. Within convective updrafts the basic charge structure has four charge regions, alternating in polarity, and the lowest is positive. Outside updrafts of convection there are typically at least six charge regions, alternating in polarity, and the lowest is again positive. Among the three storm types, there are differences in the heights and temperatures at which the basic four charge regions are found in updrafts. The height (temperature) of the center of the main negative charge region averages 6.93 km (-16 degrees C) in MCS convective region updrafts, 9.12 km (-22 degrees C) in supercell updrafts, and 6.05 km (-7 degrees C) in New Mexican mountain storm updrafts. In updraft soundings through all three storm types, the center height of the main negative charge region increases with increasing average balloon ascent rate and updraft speed at a rate of about 0.3 km per 1 m s super(-) super(1) , with a correlation coefficient of 0.94. A schematic illustrates the basic four- and six-charge structure for thunderstorm convective regions, and it is offered as an improved model for thunderstorm charge structure.</abstract></addata></record>
fulltext fulltext
identifier ISSN: 0148-0227
ispartof Journal of Geophysical Research, Washington, DC, 1998-01, Vol.103 (D12), p.14097-14108
issn 0148-0227
language eng
recordid cdi_proquest_miscellaneous_18123824
source Wiley-Blackwell AGU Digital Library
title Electrical structure in thunderstorm convective regions. Part 3: Synthesis
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-02T17%3A56%3A27IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Electrical%20structure%20in%20thunderstorm%20convective%20regions.%20Part%203:%20Synthesis&rft.jtitle=Journal%20of%20Geophysical%20Research,%20Washington,%20DC&rft.au=Stolzenburg,%20Maribeth&rft.date=1998-01-01&rft.volume=103&rft.issue=D12&rft.spage=14097&rft.epage=14108&rft.pages=14097-14108&rft.issn=0148-0227&rft_id=info:doi/&rft_dat=%3Cproquest%3E18123824%3C/proquest%3E%3Cgrp_id%3Ecdi_FETCH-proquest_miscellaneous_181238243%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=18123824&rft_id=info:pmid/&rfr_iscdi=true