Impact of Cloud-Base Turbulence on CCN Activation: Single-Size CCN
This paper examines the impact of cloud-base turbulence on activation of cloud condensation nuclei (CCN). Following our previous studies, we contrast activation within a nonturbulent adiabatic parcel and an adiabatic parcel filled with turbulence. The latter is simulated by applying a forced implici...
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Veröffentlicht in: | Journal of the atmospheric sciences 2022-02, Vol.79 (2), p.551-566 |
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description | This paper examines the impact of cloud-base turbulence on activation of cloud condensation nuclei (CCN). Following our previous studies, we contrast activation within a nonturbulent adiabatic parcel and an adiabatic parcel filled with turbulence. The latter is simulated by applying a forced implicit large-eddy simulation within a triply periodic computational domain of 64
3
m
3
. We consider two monodisperse CCN. Small CCN have a dry radius of 0.01
μ
m and a corresponding activation (critical) radius and critical supersaturation of 0.6
μ
m and 1.3%, respectively. Large CCN have a dry radius of 0.2
μ
m and feature activation radius of 5.4
μ
m and critical supersaturation 0.15%. CCN are assumed in 200-cm
−3
concentration in all cases. Mean cloud-base updraft velocities of 0.33, 1, and 3 m s
−1
are considered. In the nonturbulent parcel, all CCN are activated and lead to a monodisperse droplet size distribution above the cloud base, with practically the same droplet size in all simulations. In contrast, turbulence can lead to activation of only a fraction of all CCN with a nonzero spectral width above the cloud base, of the order of 1
μ
m, especially in the case of small CCN and weak mean cloud-base ascent. We compare our results to studies of the turbulent single-size CCN activation in the Pi chamber. Sensitivity simulations that apply a smaller turbulence intensity, smaller computational domain, and modified initial conditions document the impact of specific modeling assumptions. The simulations call for a more realistic high-resolution modeling of turbulent cloud-base activation. |
doi_str_mv | 10.1175/JAS-D-21-0184.1 |
format | Article |
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3
m
3
. We consider two monodisperse CCN. Small CCN have a dry radius of 0.01
μ
m and a corresponding activation (critical) radius and critical supersaturation of 0.6
μ
m and 1.3%, respectively. Large CCN have a dry radius of 0.2
μ
m and feature activation radius of 5.4
μ
m and critical supersaturation 0.15%. CCN are assumed in 200-cm
−3
concentration in all cases. Mean cloud-base updraft velocities of 0.33, 1, and 3 m s
−1
are considered. In the nonturbulent parcel, all CCN are activated and lead to a monodisperse droplet size distribution above the cloud base, with practically the same droplet size in all simulations. In contrast, turbulence can lead to activation of only a fraction of all CCN with a nonzero spectral width above the cloud base, of the order of 1
μ
m, especially in the case of small CCN and weak mean cloud-base ascent. We compare our results to studies of the turbulent single-size CCN activation in the Pi chamber. Sensitivity simulations that apply a smaller turbulence intensity, smaller computational domain, and modified initial conditions document the impact of specific modeling assumptions. The simulations call for a more realistic high-resolution modeling of turbulent cloud-base activation.</description><identifier>ISSN: 0022-4928</identifier><identifier>EISSN: 1520-0469</identifier><identifier>DOI: 10.1175/JAS-D-21-0184.1</identifier><language>eng</language><publisher>Boston: American Meteorological Society</publisher><subject>Adiabatic ; Adiabatic flow ; Cloud condensation nuclei ; Cloud droplet size ; Clouds ; Computer applications ; Condensation nuclei ; Domains ; Droplets ; Initial conditions ; Large eddy simulation ; Large eddy simulations ; Modelling ; Oceanic eddies ; Simulation ; Size distribution ; Supersaturation ; Turbulence ; Turbulence intensity ; Updraft</subject><ispartof>Journal of the atmospheric sciences, 2022-02, Vol.79 (2), p.551-566</ispartof><rights>Copyright American Meteorological Society Feb 2022</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c296t-769d7f94d09299ee6a4b293875fcdac102058e51dcea300d57ff875b52bf8e303</citedby><cites>FETCH-LOGICAL-c296t-769d7f94d09299ee6a4b293875fcdac102058e51dcea300d57ff875b52bf8e303</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,778,782,883,3670,27907,27908</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/1844279$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Grabowski, Wojciech W.</creatorcontrib><creatorcontrib>Thomas, Lois</creatorcontrib><creatorcontrib>Kumar, Bipin</creatorcontrib><title>Impact of Cloud-Base Turbulence on CCN Activation: Single-Size CCN</title><title>Journal of the atmospheric sciences</title><description>This paper examines the impact of cloud-base turbulence on activation of cloud condensation nuclei (CCN). Following our previous studies, we contrast activation within a nonturbulent adiabatic parcel and an adiabatic parcel filled with turbulence. The latter is simulated by applying a forced implicit large-eddy simulation within a triply periodic computational domain of 64
3
m
3
. We consider two monodisperse CCN. Small CCN have a dry radius of 0.01
μ
m and a corresponding activation (critical) radius and critical supersaturation of 0.6
μ
m and 1.3%, respectively. Large CCN have a dry radius of 0.2
μ
m and feature activation radius of 5.4
μ
m and critical supersaturation 0.15%. CCN are assumed in 200-cm
−3
concentration in all cases. Mean cloud-base updraft velocities of 0.33, 1, and 3 m s
−1
are considered. In the nonturbulent parcel, all CCN are activated and lead to a monodisperse droplet size distribution above the cloud base, with practically the same droplet size in all simulations. In contrast, turbulence can lead to activation of only a fraction of all CCN with a nonzero spectral width above the cloud base, of the order of 1
μ
m, especially in the case of small CCN and weak mean cloud-base ascent. We compare our results to studies of the turbulent single-size CCN activation in the Pi chamber. Sensitivity simulations that apply a smaller turbulence intensity, smaller computational domain, and modified initial conditions document the impact of specific modeling assumptions. The simulations call for a more realistic high-resolution modeling of turbulent cloud-base activation.</description><subject>Adiabatic</subject><subject>Adiabatic flow</subject><subject>Cloud condensation nuclei</subject><subject>Cloud droplet size</subject><subject>Clouds</subject><subject>Computer applications</subject><subject>Condensation nuclei</subject><subject>Domains</subject><subject>Droplets</subject><subject>Initial conditions</subject><subject>Large eddy simulation</subject><subject>Large eddy simulations</subject><subject>Modelling</subject><subject>Oceanic eddies</subject><subject>Simulation</subject><subject>Size distribution</subject><subject>Supersaturation</subject><subject>Turbulence</subject><subject>Turbulence intensity</subject><subject>Updraft</subject><issn>0022-4928</issn><issn>1520-0469</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNotkD1PwzAQhi0EEqUws0Ywuz07cRyztSkfRRUMLbPlODakSuMSO0jl1-Oq3HLD--jV3YPQLYEJIZxNX2drvMCUYCBFNiFnaEQYBQxZLs7RCIBSnAlaXKIr77cQh3IyQvPlbq90SJxNytYNNZ4rb5LN0FdDazptEtclZfmWzHRoflRoXPeQrJvuszV43fyaY3aNLqxqvbn532P08fS4KV_w6v15Wc5WWFORB8xzUXMrshoEFcKYXGUVFWnBmdW10gQosMIwUmujUoCacWtjWDFa2cKkkI7R3anX-dBIr5tg9Jd2XWd0kPHnjHIRofsTtO_d92B8kFs39F28S9KcszyDKCtS0xOle-d9b6zc981O9QdJQB5tymhTLiQl8mhTkvQPDpZktw</recordid><startdate>202202</startdate><enddate>202202</enddate><creator>Grabowski, Wojciech W.</creator><creator>Thomas, Lois</creator><creator>Kumar, Bipin</creator><general>American Meteorological Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>7TN</scope><scope>7UA</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>H8D</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>202202</creationdate><title>Impact of Cloud-Base Turbulence on CCN Activation: Single-Size CCN</title><author>Grabowski, Wojciech W. ; Thomas, Lois ; Kumar, Bipin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c296t-769d7f94d09299ee6a4b293875fcdac102058e51dcea300d57ff875b52bf8e303</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Adiabatic</topic><topic>Adiabatic flow</topic><topic>Cloud condensation nuclei</topic><topic>Cloud droplet size</topic><topic>Clouds</topic><topic>Computer applications</topic><topic>Condensation nuclei</topic><topic>Domains</topic><topic>Droplets</topic><topic>Initial conditions</topic><topic>Large eddy simulation</topic><topic>Large eddy simulations</topic><topic>Modelling</topic><topic>Oceanic eddies</topic><topic>Simulation</topic><topic>Size distribution</topic><topic>Supersaturation</topic><topic>Turbulence</topic><topic>Turbulence intensity</topic><topic>Updraft</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Grabowski, Wojciech W.</creatorcontrib><creatorcontrib>Thomas, Lois</creatorcontrib><creatorcontrib>Kumar, Bipin</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Journal of the atmospheric sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Grabowski, Wojciech W.</au><au>Thomas, Lois</au><au>Kumar, Bipin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Impact of Cloud-Base Turbulence on CCN Activation: Single-Size CCN</atitle><jtitle>Journal of the atmospheric sciences</jtitle><date>2022-02</date><risdate>2022</risdate><volume>79</volume><issue>2</issue><spage>551</spage><epage>566</epage><pages>551-566</pages><issn>0022-4928</issn><eissn>1520-0469</eissn><abstract>This paper examines the impact of cloud-base turbulence on activation of cloud condensation nuclei (CCN). Following our previous studies, we contrast activation within a nonturbulent adiabatic parcel and an adiabatic parcel filled with turbulence. The latter is simulated by applying a forced implicit large-eddy simulation within a triply periodic computational domain of 64
3
m
3
. We consider two monodisperse CCN. Small CCN have a dry radius of 0.01
μ
m and a corresponding activation (critical) radius and critical supersaturation of 0.6
μ
m and 1.3%, respectively. Large CCN have a dry radius of 0.2
μ
m and feature activation radius of 5.4
μ
m and critical supersaturation 0.15%. CCN are assumed in 200-cm
−3
concentration in all cases. Mean cloud-base updraft velocities of 0.33, 1, and 3 m s
−1
are considered. In the nonturbulent parcel, all CCN are activated and lead to a monodisperse droplet size distribution above the cloud base, with practically the same droplet size in all simulations. In contrast, turbulence can lead to activation of only a fraction of all CCN with a nonzero spectral width above the cloud base, of the order of 1
μ
m, especially in the case of small CCN and weak mean cloud-base ascent. We compare our results to studies of the turbulent single-size CCN activation in the Pi chamber. Sensitivity simulations that apply a smaller turbulence intensity, smaller computational domain, and modified initial conditions document the impact of specific modeling assumptions. The simulations call for a more realistic high-resolution modeling of turbulent cloud-base activation.</abstract><cop>Boston</cop><pub>American Meteorological Society</pub><doi>10.1175/JAS-D-21-0184.1</doi><tpages>16</tpages></addata></record> |
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source | American Meteorological Society; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Alma/SFX Local Collection |
subjects | Adiabatic Adiabatic flow Cloud condensation nuclei Cloud droplet size Clouds Computer applications Condensation nuclei Domains Droplets Initial conditions Large eddy simulation Large eddy simulations Modelling Oceanic eddies Simulation Size distribution Supersaturation Turbulence Turbulence intensity Updraft |
title | Impact of Cloud-Base Turbulence on CCN Activation: Single-Size CCN |
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