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contributor authorDeepak Waman
contributor authorSachin Patade
contributor authorArti Jadav
contributor authorAkash Deshmukh
contributor authorAshok Kumar Gupta
contributor authorVaughan T. J. Phillips
contributor authorAaron Bansemer
contributor authorPaul J. DeMott
date accessioned2023-04-12T18:41:18Z
date available2023-04-12T18:41:18Z
date copyright2022/12/05
date issued2022
identifier otherJAS-D-21-0278.1.pdf
identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4290073
description abstractVarious mechanisms of secondary ice production (SIP) cause multiplication of numbers of ice particle, after the onset of primary ice. A measure of SIP is the ice enhancement ratio (“IE ratio”) defined here as the ratio between number concentrations of total ice (excluding homogeneously nucleated ice) and active ice-nucleating particles (INPs). A convective line observed on 11 May 2011 over the Southern Great Plains in the Mesoscale Continental Convective Cloud Experiment (MC3E) campaign was simulated with the “Aerosol–Cloud” (AC) model. AC is validated against coincident MC3E observations by aircraft, ground-based instruments, and satellite. Four SIP mechanisms are represented in AC: the Hallett–Mossop (HM) process of rime splintering, and fragmentation during ice–ice collisions, raindrop freezing, and sublimation. The vertical profile of the IE ratio, averaged over the entire simulation, is almost uniform (10
publisherAmerican Meteorological Society
titleDependencies of Four Mechanisms of Secondary Ice Production on Cloud-Top Temperature in a Continental Convective Storm
typeJournal Paper
journal volume79
journal issue12
journal titleJournal of the Atmospheric Sciences
identifier doi10.1175/JAS-D-21-0278.1
journal fristpage3375
journal lastpage3404
page3375–3404
treeJournal of the Atmospheric Sciences:;2022:;volume( 079 ):;issue: 012
contenttypeFulltext


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