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Size‐distribution of ice crystals in cumulonimbus clouds
Author(s) -
Jones R. F.
Publication year - 1960
Publication title -
quarterly journal of the royal meteorological society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.744
H-Index - 143
eISSN - 1477-870X
pISSN - 0035-9009
DOI - 10.1002/qj.49708636808
Subject(s) - ice crystals , temperate climate , range (aeronautics) , atmospheric sciences , graupel , crystal (programming language) , physics , astrophysics , mineralogy , materials science , chemistry , meteorology , botany , composite material , biology , computer science , programming language
Ice‐crystal size‐distributions have been measured in clouds associated with the intertropical convergence zone and more isolated cumulonimbus clouds in temperate zones. Mean size‐distributions fit curves N D = 1,000/D 3 and N D = 1,000/D 2·3 in tropical and temperate clouds respectively where N D δD is the number per m 3 with diameters between D and D + δD mm. The tropical curve is a close fit throughout the measured range of D (0·05 to 4 mm) but the temperate curve is applicable in the range up to D = 2 mm only, there‐after a curve N D = 10,000/ D 5·4 fits the curve for D = 2 to 5 mm. In temperate clouds there is little variability with temperature except for a decrease in size of the largest particles observed as temperature decreases. There is some evidence that the particles caught are graupel of mean density 0·6 g cm −3 and, on this assumption, variation with total ice‐crystal concentration suggests an empirical distribution law for particles with diameters 0·25 mm or greater of \documentclass{article}\pagestyle{empty}\begin{document}$ N_D = 10^{4.1} \exp [ - \frac{{2.67}}{{W^{\frac{1}{3}} }}(D - 0.25)] $\end{document} where W is the ice‐crystal content in g m −3 .

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