Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth

<p>A novel way to represent cloud condensation nuclei (CCN) activation and cloud droplet growth by the diffusion of water vapor is introduced. The key is to apply a phase space diagram that plots the radius of a liquid droplet (deliquesced CCN or cloud droplet) versus the difference between th...

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Main Authors: W. W. Grabowski, H. Pawlowska
Format: Article
Language:English
Published: Copernicus Publications 2025-05-01
Series:Atmospheric Chemistry and Physics
Online Access:https://acp.copernicus.org/articles/25/5273/2025/acp-25-5273-2025.pdf
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author W. W. Grabowski
H. Pawlowska
author_facet W. W. Grabowski
H. Pawlowska
author_sort W. W. Grabowski
collection DOAJ
description <p>A novel way to represent cloud condensation nuclei (CCN) activation and cloud droplet growth by the diffusion of water vapor is introduced. The key is to apply a phase space diagram that plots the radius of a liquid droplet (deliquesced CCN or cloud droplet) versus the difference between the ambient supersaturation and the equilibrium supersaturation corresponding to the droplet radius. The latter combines the droplet and environmental characteristics, and it determines whether a droplet grows or evaporates. The diagram can be used to depict (in a straightforward way) key microphysical processes of CCN activation and deactivation as well as haze or cloud droplet transition from growth to evaporation. To show its utility, the diagram is applied to an idealized simulation of CCN activation and cloud droplet growth inside a rising turbulent air parcel and to simulations of microphysical processes inside a laboratory apparatus, the Pi cloud chamber. The adiabatic parcel mimics microphysical processes near the base of a natural cumulus or stratocumulus cloud. The Pi chamber simulations represent microphysical transformations in moist turbulent Rayleigh–Bénard convection with CCN proceeding through cycles of activation, growth, evaporation, and deactivation. A more general version of the phase diagram that is independent of the CCN dry radius is also developed. The phase diagram allows simple interpretations of key microphysical processes and highlights differences between droplet formation in natural and laboratory clouds.</p>
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spelling doaj-art-a2659b2ef0ef4bee88ceeaeb988938562025-08-20T03:09:03ZengCopernicus PublicationsAtmospheric Chemistry and Physics1680-73161680-73242025-05-01255273528510.5194/acp-25-5273-2025Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growthW. W. Grabowski0H. Pawlowska1MMM Laboratory, NSF National Center for Atmospheric Research, Boulder, CO, USAInstitute of Geophysics, Faculty of Physics, University of Warsaw, Warsaw, Poland<p>A novel way to represent cloud condensation nuclei (CCN) activation and cloud droplet growth by the diffusion of water vapor is introduced. The key is to apply a phase space diagram that plots the radius of a liquid droplet (deliquesced CCN or cloud droplet) versus the difference between the ambient supersaturation and the equilibrium supersaturation corresponding to the droplet radius. The latter combines the droplet and environmental characteristics, and it determines whether a droplet grows or evaporates. The diagram can be used to depict (in a straightforward way) key microphysical processes of CCN activation and deactivation as well as haze or cloud droplet transition from growth to evaporation. To show its utility, the diagram is applied to an idealized simulation of CCN activation and cloud droplet growth inside a rising turbulent air parcel and to simulations of microphysical processes inside a laboratory apparatus, the Pi cloud chamber. The adiabatic parcel mimics microphysical processes near the base of a natural cumulus or stratocumulus cloud. The Pi chamber simulations represent microphysical transformations in moist turbulent Rayleigh–Bénard convection with CCN proceeding through cycles of activation, growth, evaporation, and deactivation. A more general version of the phase diagram that is independent of the CCN dry radius is also developed. The phase diagram allows simple interpretations of key microphysical processes and highlights differences between droplet formation in natural and laboratory clouds.</p>https://acp.copernicus.org/articles/25/5273/2025/acp-25-5273-2025.pdf
spellingShingle W. W. Grabowski
H. Pawlowska
Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
Atmospheric Chemistry and Physics
title Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
title_full Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
title_fullStr Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
title_full_unstemmed Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
title_short Technical note: Phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
title_sort technical note phase space depiction of cloud condensation nuclei activation and cloud droplet diffusional growth
url https://acp.copernicus.org/articles/25/5273/2025/acp-25-5273-2025.pdf
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