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dc.contributor.authorBattan, Louis J.
dc.contributor.authorBohren, Craig F.
dc.date.accessioned2017-06-09T14:01:18Z
dc.date.available2017-06-09T14:01:18Z
dc.date.copyright1986/08/01
dc.date.issued1986
dc.identifier.issn0733-3021
dc.identifier.otherams-11036.pdf
dc.identifier.urihttp://onlinelibrary.yabesh.ir/handle/yetl/4146220
dc.description.abstractCalculations have been made of the radar backscattering and attenuation cross sections of dry and spongy ice spheres. One set of calculations was the cross sections of spheres with diameters exponentially distributed. As expected, attenuation cross sections are greater at a wavelength of 3.21 cm than at 5.05 and 10.0 cm. Calculations were also made of attenuation by monodisperse distributions of spheres composed of spongy ice and having diameters as large as about 8 cm. Attenuation of 3-cm radiation by dry ice and spongy ice spheres can be very large. At most diameters and water volume fractions, the one-way attenuation of 10-cm radiation by monodisperse spheres, in concentrations giving a radar reflectivity of 60 dBZ, is negligibly small (i.e., <0.1 dB km?1), but at a few diameters and water fractions, attenuation can be substantially larger. Although in most circumstances attenuation increases as wavelength decreases, there are exceptions at some diameters and water volume fractions. These calculations may explain observations that C-band attenuation in hailstorms is not always larger than S-band attenuation.
dc.publisherAmerican Meteorological Society
dc.titleAttenuation of Microwaves by Spherical Hail
dc.typeJournal Paper
dc.journal.volume25
dc.journal.issue8
dc.journal.titleJournal of Climate and Applied Meteorology
dc.identifier.doi10.1175/1520-0450(1986)025<1155:AOMBSH>2.0.CO;2
dc.journal.fristpage1155
dc.journal.lastpage1159
dc.treeJournal of Climate and Applied Meteorology:;1986:;Volume( 025 ):;Issue: 008
dc.contenttypeFulltext


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