The effect of secondary ice production parameterization on the simulation of a cold frontal rainband
<p>Secondary ice production via processes like rime splintering, frozen droplet shattering, and breakup upon ice hydrometeor collision have been proposed to explain discrepancies between in-cloud ice crystal and ice-nucleating particle numbers. To understand the impact of this additional i...
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doaj-82588bd7754845e99415c9581aac51472020-11-24T22:01:42ZengCopernicus PublicationsAtmospheric Chemistry and Physics1680-73161680-73242018-11-0118164611648010.5194/acp-18-16461-2018The effect of secondary ice production parameterization on the simulation of a cold frontal rainbandS. C. Sullivan0S. C. Sullivan1C. Barthlott2J. Crosier3I. Zhukov4A. Nenes5A. Nenes6A. Nenes7A. Nenes8C. Hoose9Institute of Meteorology and Climate Research, Karlsruhe Institute of Technology, Karlsruhe, GermanyDepartment of Chemical and Biomolecular Engineering, Georgia Institute of Technology, Atlanta, GA 30332, USAInstitute of Meteorology and Climate Research, Karlsruhe Institute of Technology, Karlsruhe, GermanySchool of Earth, Atmospheric, and Environmental Studies, University of Manchester, Manchester, UKJülich Supercomputing Center, Forschungszentrum Jülich, Jülich, GermanyDepartment of Chemical and Biomolecular Engineering, Georgia Institute of Technology, Atlanta, GA 30332, USAICE-HT, Foundation for Research and Technology, Hellas, 26504 Patras, GreeceInstitute of Environmental Research and Sustainable Development, National Observatory of Athens, 15236 Palea Penteli, GreeceLaboratory of Atmospheric Processes and their Impacts, School of Architecture, Civil and Environmental Engineering, École Polytechnique Fédérale de Lausanne, CH 1015, Lausanne, SwitzerlandInstitute of Meteorology and Climate Research, Karlsruhe Institute of Technology, Karlsruhe, Germany<p>Secondary ice production via processes like rime splintering, frozen droplet shattering, and breakup upon ice hydrometeor collision have been proposed to explain discrepancies between in-cloud ice crystal and ice-nucleating particle numbers. To understand the impact of this additional ice crystal generation on surface precipitation, we present one of the first studies to implement frozen droplet shattering and ice–ice collisional breakup parameterizations in a mesoscale model. We simulate a cold frontal rainband from the Aerosol Properties, PRocesses, And InfluenceS on the Earth's Climate campaign and investigate the impact of the new parameterizations on the simulated ice crystal number concentrations (ICNC) and precipitation. Near the convective regions of the rainband, contributions to ICNC can be as large from secondary production as from primary nucleation, but ICNCs greater than 50 L<sup>−1</sup> remain underestimated by the model. The addition of the secondary production parameterizations also clearly intensifies the differences in both accumulated precipitation and precipitation rate between the convective towers and non-convective gap regions. We suggest, then, that secondary ice production parameterizations be included in large-scale models on the basis of large hydrometeor concentration and convective activity criteria.</p>https://www.atmos-chem-phys.net/18/16461/2018/acp-18-16461-2018.pdf |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
S. C. Sullivan S. C. Sullivan C. Barthlott J. Crosier I. Zhukov A. Nenes A. Nenes A. Nenes A. Nenes C. Hoose |
spellingShingle |
S. C. Sullivan S. C. Sullivan C. Barthlott J. Crosier I. Zhukov A. Nenes A. Nenes A. Nenes A. Nenes C. Hoose The effect of secondary ice production parameterization on the simulation of a cold frontal rainband Atmospheric Chemistry and Physics |
author_facet |
S. C. Sullivan S. C. Sullivan C. Barthlott J. Crosier I. Zhukov A. Nenes A. Nenes A. Nenes A. Nenes C. Hoose |
author_sort |
S. C. Sullivan |
title |
The effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
title_short |
The effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
title_full |
The effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
title_fullStr |
The effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
title_full_unstemmed |
The effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
title_sort |
effect of secondary ice production parameterization on the simulation of a cold frontal rainband |
publisher |
Copernicus Publications |
series |
Atmospheric Chemistry and Physics |
issn |
1680-7316 1680-7324 |
publishDate |
2018-11-01 |
description |
<p>Secondary ice production via processes like rime splintering,
frozen droplet shattering, and breakup upon ice hydrometeor collision have
been proposed to explain discrepancies between in-cloud ice crystal and
ice-nucleating particle numbers. To understand the impact of this additional
ice crystal generation on surface precipitation, we present one of the first
studies to implement frozen droplet shattering and ice–ice collisional
breakup parameterizations in a mesoscale model. We simulate a cold frontal
rainband from the Aerosol Properties, PRocesses, And InfluenceS on the
Earth's Climate campaign and investigate the impact of the new
parameterizations on the simulated ice crystal number concentrations (ICNC)
and precipitation. Near the convective regions of the rainband, contributions
to ICNC can be as large from secondary production as from primary nucleation,
but ICNCs greater than 50 L<sup>−1</sup> remain underestimated by the model.
The addition of the secondary production parameterizations also clearly
intensifies the differences in both accumulated precipitation and
precipitation rate between the convective towers and non-convective gap
regions. We suggest, then, that secondary ice production parameterizations be
included in large-scale models on the basis of large hydrometeor
concentration and convective activity criteria.</p> |
url |
https://www.atmos-chem-phys.net/18/16461/2018/acp-18-16461-2018.pdf |
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