dc.creatorLuque, Melina Yasmín
dc.creatorBurgesser, Rodrigo Exequiel
dc.creatorCastellano, Nesvit Edit
dc.date.accessioned2021-02-15T21:17:14Z
dc.date.accessioned2022-10-15T09:04:31Z
dc.date.available2021-02-15T21:17:14Z
dc.date.available2022-10-15T09:04:31Z
dc.date.created2021-02-15T21:17:14Z
dc.date.issued2019-10
dc.identifierLuque, Melina Yasmín; Burgesser, Rodrigo Exequiel; Castellano, Nesvit Edit; Surface temperature distribution on a spherical ice particle growing by accretion in wet growth regime; John Wiley & Sons Ltd; Quarterly Journal of the Royal Meteorological Society; 145; 725; 10-2019; 3553-3560
dc.identifier0035-9009
dc.identifierhttp://hdl.handle.net/11336/125700
dc.identifier1477-870X
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4368250
dc.description.abstractExperimental evidence has demonstrated that temperature on the surface of an ice particle growing by accretion is not uniform. This non-uniformity is relevant because the ice particle surface temperature is an important microphysical parameter that influences the sign and magnitude of the charge transfer during ice particles collisions. In particular, when high values of ambient temperature and liquid water content are reached, the ice particle surface temperature is expected to reach 0 °C, which is known as wet growth regime. Previous experimental results have shown that wet growth is not uniformly reached on the ice particle surface and a surface temperature distribution is developed. In order to know the surface temperature distribution of a fixed ice particle growing by accretion of supercooled water, numerical calculations were carried out. It was found that the surface temperature distribution has a strong dependence on liquid water content, ambient temperature, airflow velocity and water droplet size. The stagnation point always reaches higher temperatures and, in many cases, its temperature is near 0 °C. For some values of the liquid water content, ambient temperature and airflow velocity, it was possible to determine temperature differences up to 7 °C between the stagnation point and the equator. This variation in the surface temperature implies that the region near the stagnation point would experience wet growth, while the rest of the ice particle surface would remain in dry growth regime, supporting the partial wet growth hypothesis. This could also explain the charge transfer reported during ice particles collisions under wet growth conditions.
dc.languageeng
dc.publisherJohn Wiley & Sons Ltd
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1002/qj.3639
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://rmets.onlinelibrary.wiley.com/doi/10.1002/qj.3639
dc.rightshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.rightsinfo:eu-repo/semantics/restrictedAccess
dc.subjectSPHERICAL ICE PARTICLE
dc.subjectSURFACE TEMPERATURE DISTRIBUTION
dc.subjectWET GROWTH
dc.titleSurface temperature distribution on a spherical ice particle growing by accretion in wet growth regime
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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