Please use this identifier to cite or link to this item:
https://physrep.ff.bg.ac.rs/handle/123456789/368
DC Field | Value | Language |
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dc.contributor.author | Ćurić, Mladjen | en |
dc.contributor.author | Janc, Dejan | en |
dc.date.accessioned | 2022-07-12T15:23:42Z | - |
dc.date.available | 2022-07-12T15:23:42Z | - |
dc.date.issued | 1991-09-01 | en |
dc.identifier.issn | 0705-5900 | en |
dc.identifier.uri | https://physrep.ff.bg.ac.rs/handle/123456789/368 | - |
dc.description.abstract | A kinematic model is applied to graupel growth. The vertical velocity and ther‐modynamic field data are taken from the forced 1‐D time‐dependent model of Cb cloud developed by Curie and Jane (1988). The graupel embryo pocket was released at the height of the — 10°C isotherm. The influence of the forced lifting on further graupel growth and its trajectory is analysed by sensitivity experiments based on the amplitude of the forced lifting, and initial graupel radius, density and cloud droplet concentration for the forced lifting initiation time derived from the model and the forced lifting duration time that agreed with observations. In particular, the sensitivity analysis was carried out for the forced lifting initiation and duration times.It is shown that for large values of the forced lifting amplitudes, the residence time of the graupel within cloud and the final graupel radius may be significantly larger compared with those in the non‐forced case. The residence time in a cloud can also be significantly larger for the smallest amplitude, whereas the final radius is rather insensitive owing to oscillations around the melting level. For some cases the forced lifting causes recycling inside the updraft, contrary to the results of previous non‐forced numerical models. The recycling mechanism is sensitive to the forced lifting duration time and the time interval between the graupel pocket injection in cloud and the initiation of the forced lifting. Initially the observed recycling mechanism is a consequence of the periodic forced lifting mechanism, but then combines with recycling of the Pflaum type (1980). © 1991 Taylor & Francis Group, LLC. | en |
dc.relation.ispartof | Atmosphere - Ocean | en |
dc.title | Graupel growth and trajectories in a shallow CB cloud determined by a forced 1‐D model | en |
dc.type | Article | en |
dc.identifier.doi | 10.1080/07055900.1991.9649413 | en |
dc.identifier.scopus | 2-s2.0-5544220060 | en |
dc.identifier.url | https://api.elsevier.com/content/abstract/scopus_id/5544220060 | en |
dc.relation.issue | 3 | en |
dc.relation.volume | 29 | en |
dc.relation.firstpage | 462 | en |
dc.relation.lastpage | 478 | en |
item.openairetype | Article | - |
item.cerifentitytype | Publications | - |
item.fulltext | No Fulltext | - |
item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
item.grantfulltext | none | - |
Appears in Collections: | Journal Article |
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