Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7

<p>Large-eddy simulation (LES) models are an excellent tool to improve our understanding of aerosol–cloud interactions (ACI). We introduce a prognostic aerosol scheme with multiple aerosol species in the Dutch Atmospheric Large-Eddy Simulation model (DALES), especially focused on simulating th...

Full description

Bibliographic Details
Main Authors: M. de Bruine, M. Krol, J. Vilà-Guerau de Arellano, T. Röckmann
Format: Article
Language:English
Published: Copernicus Publications 2019-12-01
Series:Geoscientific Model Development
Online Access:https://www.geosci-model-dev.net/12/5177/2019/gmd-12-5177-2019.pdf
id doaj-d541c9968ab64b45ba4c351996a17ba9
record_format Article
spelling doaj-d541c9968ab64b45ba4c351996a17ba92020-11-25T01:51:07ZengCopernicus PublicationsGeoscientific Model Development1991-959X1991-96032019-12-01125177519610.5194/gmd-12-5177-2019Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7M. de Bruine0M. de Bruine1M. Krol2M. Krol3J. Vilà-Guerau de Arellano4T. Röckmann5Institute for Marine and Atmospheric Research Utrecht, Utrecht University, Utrecht, the NetherlandsDepartment of Meteorology and Air Quality, Wageningen University, Wageningen, the NetherlandsInstitute for Marine and Atmospheric Research Utrecht, Utrecht University, Utrecht, the NetherlandsDepartment of Meteorology and Air Quality, Wageningen University, Wageningen, the NetherlandsDepartment of Meteorology and Air Quality, Wageningen University, Wageningen, the NetherlandsInstitute for Marine and Atmospheric Research Utrecht, Utrecht University, Utrecht, the Netherlands<p>Large-eddy simulation (LES) models are an excellent tool to improve our understanding of aerosol–cloud interactions (ACI). We introduce a prognostic aerosol scheme with multiple aerosol species in the Dutch Atmospheric Large-Eddy Simulation model (DALES), especially focused on simulating the impact of cloud microphysical processes on the aerosol population. The numerical treatment of aerosol activation is a crucial element for simulating both cloud and aerosol characteristics. Two methods are implemented and discussed: an explicit activation scheme based on <span class="inline-formula"><i>κ</i></span>-Köhler theory and a more classic approach using updraught strength. Sample model simulations are based on the Rain in Shallow Cumulus over the Ocean (RICO) campaign, characterized by rapidly precipitating warm-phase shallow cumulus clouds.</p> <p>We find that in this pristine ocean environment virtually all aerosol mass in cloud droplets is the result of the activation process, while in-cloud scavenging is relatively inefficient. Despite the rapid formation of precipitation, most of the in-cloud aerosol mass is returned to the atmosphere by cloud evaporation. The strength of aerosol processing through subsequent cloud cycles is found to be particularly sensitive to the activation scheme and resulting cloud characteristics. However, the precipitation processes are considerably less sensitive. Scavenging by precipitation is the dominant source for in-rain aerosol mass. About half of the in-rain aerosol reaches the surface, while the rest is released by evaporation of falling precipitation. The effect of cloud microphysics on the average aerosol size depends on the balance between the evaporation of clouds and rain and ultimate removal by precipitation. Analysis of typical aerosol size associated with the different microphysical processes shows that aerosols resuspended by cloud evaporation have a radius that is only 5&thinsp;% to 10&thinsp;% larger than the originally activated aerosols. In contrast, aerosols released by evaporating precipitation are an order of magnitude larger.</p>https://www.geosci-model-dev.net/12/5177/2019/gmd-12-5177-2019.pdf
collection DOAJ
language English
format Article
sources DOAJ
author M. de Bruine
M. de Bruine
M. Krol
M. Krol
J. Vilà-Guerau de Arellano
T. Röckmann
spellingShingle M. de Bruine
M. de Bruine
M. Krol
M. Krol
J. Vilà-Guerau de Arellano
T. Röckmann
Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
Geoscientific Model Development
author_facet M. de Bruine
M. de Bruine
M. Krol
M. Krol
J. Vilà-Guerau de Arellano
T. Röckmann
author_sort M. de Bruine
title Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
title_short Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
title_full Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
title_fullStr Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
title_full_unstemmed Explicit aerosol–cloud interactions in the Dutch Atmospheric Large-Eddy Simulation model DALES4.1-M7
title_sort explicit aerosol–cloud interactions in the dutch atmospheric large-eddy simulation model dales4.1-m7
publisher Copernicus Publications
series Geoscientific Model Development
issn 1991-959X
1991-9603
publishDate 2019-12-01
description <p>Large-eddy simulation (LES) models are an excellent tool to improve our understanding of aerosol–cloud interactions (ACI). We introduce a prognostic aerosol scheme with multiple aerosol species in the Dutch Atmospheric Large-Eddy Simulation model (DALES), especially focused on simulating the impact of cloud microphysical processes on the aerosol population. The numerical treatment of aerosol activation is a crucial element for simulating both cloud and aerosol characteristics. Two methods are implemented and discussed: an explicit activation scheme based on <span class="inline-formula"><i>κ</i></span>-Köhler theory and a more classic approach using updraught strength. Sample model simulations are based on the Rain in Shallow Cumulus over the Ocean (RICO) campaign, characterized by rapidly precipitating warm-phase shallow cumulus clouds.</p> <p>We find that in this pristine ocean environment virtually all aerosol mass in cloud droplets is the result of the activation process, while in-cloud scavenging is relatively inefficient. Despite the rapid formation of precipitation, most of the in-cloud aerosol mass is returned to the atmosphere by cloud evaporation. The strength of aerosol processing through subsequent cloud cycles is found to be particularly sensitive to the activation scheme and resulting cloud characteristics. However, the precipitation processes are considerably less sensitive. Scavenging by precipitation is the dominant source for in-rain aerosol mass. About half of the in-rain aerosol reaches the surface, while the rest is released by evaporation of falling precipitation. The effect of cloud microphysics on the average aerosol size depends on the balance between the evaporation of clouds and rain and ultimate removal by precipitation. Analysis of typical aerosol size associated with the different microphysical processes shows that aerosols resuspended by cloud evaporation have a radius that is only 5&thinsp;% to 10&thinsp;% larger than the originally activated aerosols. In contrast, aerosols released by evaporating precipitation are an order of magnitude larger.</p>
url https://www.geosci-model-dev.net/12/5177/2019/gmd-12-5177-2019.pdf
work_keys_str_mv AT mdebruine explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
AT mdebruine explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
AT mkrol explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
AT mkrol explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
AT jvilagueraudearellano explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
AT trockmann explicitaerosolcloudinteractionsinthedutchatmosphericlargeeddysimulationmodeldales41m7
_version_ 1724998458220216320