Eddy kinetic energy redistribution within windstorms Klaus and Friedhelm
The formation of lower‐tropospheric wind speed maxima is analyzed during the mature stage of two distinct windstorms using ERA‐Interim reanalysis datasets and performing an eddy kinetic energy (EKE) budget. Both storms developed according to the Shapiro–Keyser conceptual model and crossed the large‐...
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Veröffentlicht in: | Quarterly journal of the Royal Meteorological Society 2015-04, Vol.141 (688), p.925-938 |
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description | The formation of lower‐tropospheric wind speed maxima is analyzed during the mature stage of two distinct windstorms using ERA‐Interim reanalysis datasets and performing an eddy kinetic energy (EKE) budget. Both storms developed according to the Shapiro–Keyser conceptual model and crossed the large‐scale low‐frequency jet from its warm‐air towards its cold‐air side. The formation of strong wind regions are shown to depend on the position of the storms relative to the large‐scale jet axis, which confirm theoretical results of a companion study. As long as the storms are travelling south of the low‐frequency jet or close to the jet axis, the most intense EKE maxima as well as the total kinetic energy maxima are located in the warm sector of the surface cyclones on their southeastern side. As soon as the surface cyclones move to the north of the low‐frequency jet, EKE is cyclonically redistributed in the lower troposphere, first to the northnorthwest of the cyclone's centre, and then to the southwest along the bent‐back warm fronts. At this later stage, EKE, which is generated by baroclinic conversion in the mid‐troposphere, is redistributed downwards by the vertical ageostrophic geopotential fluxes before being further redistributed southwestwards in the lower troposphere by the ageostrophic geopotential fluxes. This EKE redistribution led to the formation of a low‐level westerly jet to the south of each cyclone centre behind the cold front. These common features between the two storms happened in spite of differences in their shape and environment. |
doi_str_mv | 10.1002/qj.2412 |
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Both storms developed according to the Shapiro–Keyser conceptual model and crossed the large‐scale low‐frequency jet from its warm‐air towards its cold‐air side. The formation of strong wind regions are shown to depend on the position of the storms relative to the large‐scale jet axis, which confirm theoretical results of a companion study. As long as the storms are travelling south of the low‐frequency jet or close to the jet axis, the most intense EKE maxima as well as the total kinetic energy maxima are located in the warm sector of the surface cyclones on their southeastern side. As soon as the surface cyclones move to the north of the low‐frequency jet, EKE is cyclonically redistributed in the lower troposphere, first to the northnorthwest of the cyclone's centre, and then to the southwest along the bent‐back warm fronts. At this later stage, EKE, which is generated by baroclinic conversion in the mid‐troposphere, is redistributed downwards by the vertical ageostrophic geopotential fluxes before being further redistributed southwestwards in the lower troposphere by the ageostrophic geopotential fluxes. This EKE redistribution led to the formation of a low‐level westerly jet to the south of each cyclone centre behind the cold front. These common features between the two storms happened in spite of differences in their shape and environment.</description><identifier>ISSN: 0035-9009</identifier><identifier>EISSN: 1477-870X</identifier><identifier>DOI: 10.1002/qj.2412</identifier><language>eng</language><publisher>Chichester, UK: John Wiley & Sons, Ltd</publisher><subject>Brackish ; Cyclones ; Eddies ; eddy kinetic energy ; Energy ; Fluxes ; Formations ; jet crossing ; Kinetic energy ; Marine ; Maxima ; Meteorology ; Storms ; Troposphere ; windstorms</subject><ispartof>Quarterly journal of the Royal Meteorological Society, 2015-04, Vol.141 (688), p.925-938</ispartof><rights>2014 Royal Meteorological Society</rights><rights>2015 Royal Meteorological Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3882-4f1a3d05ff21d1e9544c2254eff7fea6330ce0ce3325d0a4a5e1d957ee785c373</citedby><cites>FETCH-LOGICAL-c3882-4f1a3d05ff21d1e9544c2254eff7fea6330ce0ce3325d0a4a5e1d957ee785c373</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fqj.2412$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fqj.2412$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,776,780,1411,27903,27904,45553,45554</link.rule.ids></links><search><creatorcontrib>Rivière, G.</creatorcontrib><creatorcontrib>Arbogast, P.</creatorcontrib><creatorcontrib>Joly, A.</creatorcontrib><title>Eddy kinetic energy redistribution within windstorms Klaus and Friedhelm</title><title>Quarterly journal of the Royal Meteorological Society</title><description>The formation of lower‐tropospheric wind speed maxima is analyzed during the mature stage of two distinct windstorms using ERA‐Interim reanalysis datasets and performing an eddy kinetic energy (EKE) budget. Both storms developed according to the Shapiro–Keyser conceptual model and crossed the large‐scale low‐frequency jet from its warm‐air towards its cold‐air side. The formation of strong wind regions are shown to depend on the position of the storms relative to the large‐scale jet axis, which confirm theoretical results of a companion study. As long as the storms are travelling south of the low‐frequency jet or close to the jet axis, the most intense EKE maxima as well as the total kinetic energy maxima are located in the warm sector of the surface cyclones on their southeastern side. As soon as the surface cyclones move to the north of the low‐frequency jet, EKE is cyclonically redistributed in the lower troposphere, first to the northnorthwest of the cyclone's centre, and then to the southwest along the bent‐back warm fronts. At this later stage, EKE, which is generated by baroclinic conversion in the mid‐troposphere, is redistributed downwards by the vertical ageostrophic geopotential fluxes before being further redistributed southwestwards in the lower troposphere by the ageostrophic geopotential fluxes. This EKE redistribution led to the formation of a low‐level westerly jet to the south of each cyclone centre behind the cold front. These common features between the two storms happened in spite of differences in their shape and environment.</description><subject>Brackish</subject><subject>Cyclones</subject><subject>Eddies</subject><subject>eddy kinetic energy</subject><subject>Energy</subject><subject>Fluxes</subject><subject>Formations</subject><subject>jet crossing</subject><subject>Kinetic energy</subject><subject>Marine</subject><subject>Maxima</subject><subject>Meteorology</subject><subject>Storms</subject><subject>Troposphere</subject><subject>windstorms</subject><issn>0035-9009</issn><issn>1477-870X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqN0EtLw0AUBeBBFKxV_AsBFwqSeufVSZZSWqsWRFBwF8bMjZ2YRzuTUPLvTawrQRAunM3HgXsIOacwoQDsZptPmKDsgIyoUCqMFLwdkhEAl2EMEB-TE-9zAJCKqRFZzo3pgk9bYWPTACt0H13g0FjfOPveNraugp1t1naIyvimdqUPHgvd-kBXJlg4i2aNRXlKjjJdeDz7yTF5XcxfZstw9XR3P7tdhSmPIhaKjGpuQGYZo4ZiLIVIGZMCs0xlqKecQ4r9cc6kAS20RGpiqRBVJFOu-Jhc7Xs3rt626JuktD7FotAV1q1P6DRmAiSV4h80AiHjfqWeXvyied26qn-kV2oKsVJiUJd7lbrae4dZsnG21K5LKCTD-Mk2T4bxe3m9lztbYPcXS54fvvUXTeyDkw</recordid><startdate>201504</startdate><enddate>201504</enddate><creator>Rivière, G.</creator><creator>Arbogast, P.</creator><creator>Joly, A.</creator><general>John Wiley & Sons, Ltd</general><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>7TN</scope><scope>F1W</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><scope>7UA</scope><scope>C1K</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>201504</creationdate><title>Eddy kinetic energy redistribution within windstorms Klaus and Friedhelm</title><author>Rivière, G. ; Arbogast, P. ; Joly, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3882-4f1a3d05ff21d1e9544c2254eff7fea6330ce0ce3325d0a4a5e1d957ee785c373</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Brackish</topic><topic>Cyclones</topic><topic>Eddies</topic><topic>eddy kinetic energy</topic><topic>Energy</topic><topic>Fluxes</topic><topic>Formations</topic><topic>jet crossing</topic><topic>Kinetic energy</topic><topic>Marine</topic><topic>Maxima</topic><topic>Meteorology</topic><topic>Storms</topic><topic>Troposphere</topic><topic>windstorms</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rivière, G.</creatorcontrib><creatorcontrib>Arbogast, P.</creatorcontrib><creatorcontrib>Joly, A.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Quarterly journal of the Royal Meteorological Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Rivière, G.</au><au>Arbogast, P.</au><au>Joly, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Eddy kinetic energy redistribution within windstorms Klaus and Friedhelm</atitle><jtitle>Quarterly journal of the Royal Meteorological Society</jtitle><date>2015-04</date><risdate>2015</risdate><volume>141</volume><issue>688</issue><spage>925</spage><epage>938</epage><pages>925-938</pages><issn>0035-9009</issn><eissn>1477-870X</eissn><abstract>The formation of lower‐tropospheric wind speed maxima is analyzed during the mature stage of two distinct windstorms using ERA‐Interim reanalysis datasets and performing an eddy kinetic energy (EKE) budget. Both storms developed according to the Shapiro–Keyser conceptual model and crossed the large‐scale low‐frequency jet from its warm‐air towards its cold‐air side. The formation of strong wind regions are shown to depend on the position of the storms relative to the large‐scale jet axis, which confirm theoretical results of a companion study. As long as the storms are travelling south of the low‐frequency jet or close to the jet axis, the most intense EKE maxima as well as the total kinetic energy maxima are located in the warm sector of the surface cyclones on their southeastern side. As soon as the surface cyclones move to the north of the low‐frequency jet, EKE is cyclonically redistributed in the lower troposphere, first to the northnorthwest of the cyclone's centre, and then to the southwest along the bent‐back warm fronts. At this later stage, EKE, which is generated by baroclinic conversion in the mid‐troposphere, is redistributed downwards by the vertical ageostrophic geopotential fluxes before being further redistributed southwestwards in the lower troposphere by the ageostrophic geopotential fluxes. This EKE redistribution led to the formation of a low‐level westerly jet to the south of each cyclone centre behind the cold front. These common features between the two storms happened in spite of differences in their shape and environment.</abstract><cop>Chichester, UK</cop><pub>John Wiley & Sons, Ltd</pub><doi>10.1002/qj.2412</doi><tpages>14</tpages></addata></record> |
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subjects | Brackish Cyclones Eddies eddy kinetic energy Energy Fluxes Formations jet crossing Kinetic energy Marine Maxima Meteorology Storms Troposphere windstorms |
title | Eddy kinetic energy redistribution within windstorms Klaus and Friedhelm |
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