Main Detrainment Height of Deep Convection Systems over the Tibetan Plateau and Its Southern Slope
Deep convection systems (DCSs) can rapidly lift water vapor and other pollutants from the lower troposphere to the upper troposphere and lower stratosphere. The main detrainment height determines the level to which the air parcel is lifted. We analyzed the main detrainment height over the Tibetan Pl...
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description | Deep convection systems (DCSs) can rapidly lift water vapor and other pollutants from the lower troposphere to the upper troposphere and lower stratosphere. The main detrainment height determines the level to which the air parcel is lifted. We analyzed the main detrainment height over the Tibetan Plateau and its southern slope based on the CloudSat Cloud Profiling Radar 2B_GEOPROF dataset and the Aura Microwave Limb Sounder Level 2 cloud ice product onboard the A-train constellation of Earth-observing satellites. It was found that the DCSs over the Tibetan Plateau and its southern slope have a higher main detrainment height (about 10–16 km) than other regions in the same latitude. The mean main detrainment heights are 12.9 and 13.3 km over the Tibetan Plateau and its southern slope, respectively. The cloud ice water path decreases by 16.8% after excluding the influences of DCSs, and the height with the maximum increase in cloud ice water content is located at 178 hPa (about 13 km). The main detrainment height and outflow horizontal range are higher and larger over the central and eastern Tibetan Plateau, the west of the southern slope, and the southeastern edge of the Tibetan Plateau than that over the northwestern Tibetan Plateau. The main detrainment height and outflow horizontal range are lower and broader at nighttime than during daytime. |
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The main detrainment height determines the level to which the air parcel is lifted. We analyzed the main detrainment height over the Tibetan Plateau and its southern slope based on the CloudSat Cloud Profiling Radar 2B_GEOPROF dataset and the Aura Microwave Limb Sounder Level 2 cloud ice product onboard the A-train constellation of Earth-observing satellites. It was found that the DCSs over the Tibetan Plateau and its southern slope have a higher main detrainment height (about 10–16 km) than other regions in the same latitude. The mean main detrainment heights are 12.9 and 13.3 km over the Tibetan Plateau and its southern slope, respectively. The cloud ice water path decreases by 16.8% after excluding the influences of DCSs, and the height with the maximum increase in cloud ice water content is located at 178 hPa (about 13 km). The main detrainment height and outflow horizontal range are higher and larger over the central and eastern Tibetan Plateau, the west of the southern slope, and the southeastern edge of the Tibetan Plateau than that over the northwestern Tibetan Plateau. The main detrainment height and outflow horizontal range are lower and broader at nighttime than during daytime.</description><identifier>ISSN: 0256-1530</identifier><identifier>EISSN: 1861-9533</identifier><identifier>DOI: 10.1007/s00376-019-9003-3</identifier><language>eng</language><publisher>Heidelberg: Science Press</publisher><subject>Air parcels ; Atmospheric Sciences ; Clouds ; Convection ; Detrainment ; Earth ; Earth and Environmental Science ; Earth Sciences ; Geophysics/Geodesy ; Height ; Ice ; Lower stratosphere ; Lower troposphere ; Meteorology ; Moisture content ; Original Paper ; Outflow ; Plateaus ; Pollutants ; Radar ; Satellite constellations ; Satellite observation ; Slopes ; Stratosphere ; Troposphere ; Upper troposphere ; Water content ; Water pollution ; Water vapor ; Water vapour</subject><ispartof>Advances in atmospheric sciences, 2019-10, Vol.36 (10), p.1078-1088</ispartof><rights>Institute of Atmospheric Physics/Chinese Academy of Sciences, and Science Press and Springer-Verlag GmbH Germany, part of Springer Nature 2019</rights><rights>Copyright Springer Nature B.V. 2019</rights><rights>Copyright © Wanfang Data Co. Ltd. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c350t-d2ecc21380e0fe38ddf234dc23f3575798485de78cff3de22fca601221490f73</citedby><cites>FETCH-LOGICAL-c350t-d2ecc21380e0fe38ddf234dc23f3575798485de78cff3de22fca601221490f73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://www.wanfangdata.com.cn/images/PeriodicalImages/dqkxjz-e/dqkxjz-e.jpg</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s00376-019-9003-3$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s00376-019-9003-3$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Chen, Quanliang</creatorcontrib><creatorcontrib>Gao, Guolu</creatorcontrib><creatorcontrib>Li, Yang</creatorcontrib><creatorcontrib>Cai, Hongke</creatorcontrib><creatorcontrib>Zhou, Xin</creatorcontrib><creatorcontrib>Wang, Zhenglin</creatorcontrib><title>Main Detrainment Height of Deep Convection Systems over the Tibetan Plateau and Its Southern Slope</title><title>Advances in atmospheric sciences</title><addtitle>Adv. Atmos. Sci</addtitle><description>Deep convection systems (DCSs) can rapidly lift water vapor and other pollutants from the lower troposphere to the upper troposphere and lower stratosphere. The main detrainment height determines the level to which the air parcel is lifted. We analyzed the main detrainment height over the Tibetan Plateau and its southern slope based on the CloudSat Cloud Profiling Radar 2B_GEOPROF dataset and the Aura Microwave Limb Sounder Level 2 cloud ice product onboard the A-train constellation of Earth-observing satellites. It was found that the DCSs over the Tibetan Plateau and its southern slope have a higher main detrainment height (about 10–16 km) than other regions in the same latitude. The mean main detrainment heights are 12.9 and 13.3 km over the Tibetan Plateau and its southern slope, respectively. The cloud ice water path decreases by 16.8% after excluding the influences of DCSs, and the height with the maximum increase in cloud ice water content is located at 178 hPa (about 13 km). The main detrainment height and outflow horizontal range are higher and larger over the central and eastern Tibetan Plateau, the west of the southern slope, and the southeastern edge of the Tibetan Plateau than that over the northwestern Tibetan Plateau. The main detrainment height and outflow horizontal range are lower and broader at nighttime than during daytime.</description><subject>Air parcels</subject><subject>Atmospheric Sciences</subject><subject>Clouds</subject><subject>Convection</subject><subject>Detrainment</subject><subject>Earth</subject><subject>Earth and Environmental Science</subject><subject>Earth Sciences</subject><subject>Geophysics/Geodesy</subject><subject>Height</subject><subject>Ice</subject><subject>Lower stratosphere</subject><subject>Lower troposphere</subject><subject>Meteorology</subject><subject>Moisture content</subject><subject>Original Paper</subject><subject>Outflow</subject><subject>Plateaus</subject><subject>Pollutants</subject><subject>Radar</subject><subject>Satellite constellations</subject><subject>Satellite observation</subject><subject>Slopes</subject><subject>Stratosphere</subject><subject>Troposphere</subject><subject>Upper troposphere</subject><subject>Water content</subject><subject>Water pollution</subject><subject>Water vapor</subject><subject>Water vapour</subject><issn>0256-1530</issn><issn>1861-9533</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp1kMtOAjEUhhujiYg-gLsmrlyM9jLXpcELJBhNYN-UzikMQju0BcWntzgmrFydk9Pv_5t8CF1TckcJKe49IbzIE0KrpIprwk9Qj5Y5TaqM81PUIyzLE5pxco4uvF9GpOIl7aHZq2wMfoTg4lyDCXgIzXwRsNXxCi0eWLMDFRpr8GTvA6w9tjtwOCwAT5sZBGnw-0oGkFssTY1HweOJ3cZnFxMr28IlOtNy5eHqb_bR9PlpOhgm47eX0eBhnCiekZDUDJRilJcEiAZe1rVmPK0V45pnRVZUZVpmNRSl0prXwJhWMieUMZpWRBe8j2672k9ptDRzsbRbZ-KHot58fC2_BbBoJ8oiPLI3Hds6u9mCD0eYseK3NUsjRTtKOeu9Ay1a16yl2wtKxMG66KyL2CsO1sWhmXUZH1kzB3ds_j_0A1XRhBk</recordid><startdate>20191001</startdate><enddate>20191001</enddate><creator>Chen, Quanliang</creator><creator>Gao, Guolu</creator><creator>Li, Yang</creator><creator>Cai, Hongke</creator><creator>Zhou, Xin</creator><creator>Wang, Zhenglin</creator><general>Science Press</general><general>Springer Nature B.V</general><general>School of Atmospheric Sciences, Chengdu University of Information Technology and Plateau Atmosphere and Environment Key Laboratory of Sichuan Province, Chengdu 610225, China</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>F1W</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><scope>2B.</scope><scope>4A8</scope><scope>92I</scope><scope>93N</scope><scope>PSX</scope><scope>TCJ</scope></search><sort><creationdate>20191001</creationdate><title>Main Detrainment Height of Deep Convection Systems over the Tibetan Plateau and Its Southern Slope</title><author>Chen, Quanliang ; Gao, Guolu ; Li, Yang ; Cai, Hongke ; Zhou, Xin ; Wang, Zhenglin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c350t-d2ecc21380e0fe38ddf234dc23f3575798485de78cff3de22fca601221490f73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Air parcels</topic><topic>Atmospheric Sciences</topic><topic>Clouds</topic><topic>Convection</topic><topic>Detrainment</topic><topic>Earth</topic><topic>Earth and Environmental Science</topic><topic>Earth Sciences</topic><topic>Geophysics/Geodesy</topic><topic>Height</topic><topic>Ice</topic><topic>Lower stratosphere</topic><topic>Lower troposphere</topic><topic>Meteorology</topic><topic>Moisture content</topic><topic>Original Paper</topic><topic>Outflow</topic><topic>Plateaus</topic><topic>Pollutants</topic><topic>Radar</topic><topic>Satellite constellations</topic><topic>Satellite observation</topic><topic>Slopes</topic><topic>Stratosphere</topic><topic>Troposphere</topic><topic>Upper troposphere</topic><topic>Water content</topic><topic>Water pollution</topic><topic>Water vapor</topic><topic>Water vapour</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chen, Quanliang</creatorcontrib><creatorcontrib>Gao, Guolu</creatorcontrib><creatorcontrib>Li, Yang</creatorcontrib><creatorcontrib>Cai, Hongke</creatorcontrib><creatorcontrib>Zhou, Xin</creatorcontrib><creatorcontrib>Wang, Zhenglin</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical 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>Wanfang Data Journals - Hong Kong</collection><collection>WANFANG Data Centre</collection><collection>Wanfang Data Journals</collection><collection>万方数据期刊 - 香港版</collection><collection>China Online Journals (COJ)</collection><collection>China Online Journals (COJ)</collection><jtitle>Advances in atmospheric sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chen, Quanliang</au><au>Gao, Guolu</au><au>Li, Yang</au><au>Cai, Hongke</au><au>Zhou, Xin</au><au>Wang, Zhenglin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Main Detrainment Height of Deep Convection Systems over the Tibetan Plateau and Its Southern Slope</atitle><jtitle>Advances in atmospheric sciences</jtitle><stitle>Adv. Atmos. Sci</stitle><date>2019-10-01</date><risdate>2019</risdate><volume>36</volume><issue>10</issue><spage>1078</spage><epage>1088</epage><pages>1078-1088</pages><issn>0256-1530</issn><eissn>1861-9533</eissn><abstract>Deep convection systems (DCSs) can rapidly lift water vapor and other pollutants from the lower troposphere to the upper troposphere and lower stratosphere. The main detrainment height determines the level to which the air parcel is lifted. We analyzed the main detrainment height over the Tibetan Plateau and its southern slope based on the CloudSat Cloud Profiling Radar 2B_GEOPROF dataset and the Aura Microwave Limb Sounder Level 2 cloud ice product onboard the A-train constellation of Earth-observing satellites. It was found that the DCSs over the Tibetan Plateau and its southern slope have a higher main detrainment height (about 10–16 km) than other regions in the same latitude. The mean main detrainment heights are 12.9 and 13.3 km over the Tibetan Plateau and its southern slope, respectively. The cloud ice water path decreases by 16.8% after excluding the influences of DCSs, and the height with the maximum increase in cloud ice water content is located at 178 hPa (about 13 km). The main detrainment height and outflow horizontal range are higher and larger over the central and eastern Tibetan Plateau, the west of the southern slope, and the southeastern edge of the Tibetan Plateau than that over the northwestern Tibetan Plateau. The main detrainment height and outflow horizontal range are lower and broader at nighttime than during daytime.</abstract><cop>Heidelberg</cop><pub>Science Press</pub><doi>10.1007/s00376-019-9003-3</doi><tpages>11</tpages></addata></record> |
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subjects | Air parcels Atmospheric Sciences Clouds Convection Detrainment Earth Earth and Environmental Science Earth Sciences Geophysics/Geodesy Height Ice Lower stratosphere Lower troposphere Meteorology Moisture content Original Paper Outflow Plateaus Pollutants Radar Satellite constellations Satellite observation Slopes Stratosphere Troposphere Upper troposphere Water content Water pollution Water vapor Water vapour |
title | Main Detrainment Height of Deep Convection Systems over the Tibetan Plateau and Its Southern Slope |
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