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dc.contributor.authorAtlas, David
dc.contributor.authorBartnoff, Shepard
dc.date.accessioned2017-06-09T14:10:43Z
dc.date.available2017-06-09T14:10:43Z
dc.date.copyright1953/04/01
dc.date.issued1953
dc.identifier.issn0095-9634
dc.identifier.otherams-13974.pdf
dc.identifier.urihttp://onlinelibrary.yabesh.ir/handle/yetl/4149483
dc.description.abstractThe coefficient C in Trabert's visibility equation, V = (C?r?)/W, where r? is linear mean radius, ? density, and W is liquid-water content, is shown to be a function of the breadth of the drop-size distribution but has preferred values in natural clouds ranging from 3.3 for fair-weather cumulus to 4.8 for nimbostratus. The frequently quoted value of 2.6 pertains only to a perfectly monodisperse distribution, and is inappropriate in nature. A more useful equation is found to be V = (K?d0)/W, in which >d0 is the median volume diameter and the coefficient K is found to be very nearly independent of the breadth of the drop-size spectrum over the range which occurs in natural clouds. K = 1.2 is shown to be an excellent value for 65 observations by Diem. Similarly, the coefficient G in the radar-reflectivity equation, Z = (6/π)G d03(W/?) ? 10?6 has a preferred value of 1.35. The implication is that nature has a preference for a particular type of drop-size spectrum.
dc.publisherAmerican Meteorological Society
dc.titleCLOUD VISIBILITY, RADAR REFLECTIVITY, AND DROP-SIZE DISTRIBUTION
dc.typeJournal Paper
dc.journal.volume10
dc.journal.issue2
dc.journal.titleJournal of Meteorology
dc.identifier.doi10.1175/1520-0469(1953)010<0143:CVRRAD>2.0.CO;2
dc.journal.fristpage143
dc.journal.lastpage148
dc.treeJournal of Meteorology:;1953:;volume( 010 ):;issue: 002
dc.contenttypeFulltext


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