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dc.contributor.authorWilde, Nicholas P.
dc.contributor.authorStull, Roland B.
dc.contributor.authorEloranta, Edwin W.
dc.date.accessioned2017-06-09T14:00:40Z
dc.date.available2017-06-09T14:00:40Z
dc.date.copyright1985/07/01
dc.date.issued1985
dc.identifier.issn0733-3021
dc.identifier.otherams-10864.pdf
dc.identifier.urihttp://onlinelibrary.yabesh.ir/handle/yetl/4146028
dc.description.abstractVariations of the lifting condensation level (LCL) of surface layer air are documented based on data from the BLX83 field experiment in Oklahoma. For example, within a 25 km long region near Chickasha, the local LCL height was found to vary by 15?30% of its average height. This zone of variation, centered on the mean LCL height, is identified as the ?LCL zone?. It is analogous to the entrainment zone for the local mixed layer depth. Cumulus clouds first form when the top of the entrainment zone reaches the bottom of the LCL zone. As more of the entrainment zone overlaps and reaches above the LCL zone, the cloud cover increases. Two case studies are presented to demonstrate the diagnosis of cumulus onset time and cloud cover amount using this overlap technique. Combined radar, aircraft, rawinsonde, and surface observations indicate that some of the air observed at cloud base has the same low LCL as that of the mean surface layer air. This leads us to speculate that some surface layer air is rising up to cloud base with relatively little dilution, perhaps within the cores of thermals.
dc.publisherAmerican Meteorological Society
dc.titleThe LCL Zone and Cumulus Onset
dc.typeJournal Paper
dc.journal.volume24
dc.journal.issue7
dc.journal.titleJournal of Climate and Applied Meteorology
dc.identifier.doi10.1175/1520-0450(1985)024<0640:TLZACO>2.0.CO;2
dc.journal.fristpage640
dc.journal.lastpage657
dc.treeJournal of Climate and Applied Meteorology:;1985:;Volume( 024 ):;Issue: 007
dc.contenttypeFulltext


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