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    Virtual Field Campaigns on Deep Tropical Convection in Climate Models

    Source: Journal of Climate:;2009:;volume( 022 ):;issue: 002::page 244
    Author:
    Mapes, Brian
    ,
    Bacmeister, Julio
    ,
    Khairoutdinov, Marat
    ,
    Hannay, Cecile
    ,
    Zhao, Ming
    DOI: 10.1175/2008JCLI2203.1
    Publisher: American Meteorological Society
    Abstract: High-resolution time?height data over warm tropical oceans are examined, from three global atmosphere models [GFDL?s Atmosphere Model 2 (AM2), NCAR?s Community Atmosphere Model, version 3 (CAM3), and a NASA Global Modeling and Assimilation Office (GMAO) model], field campaign observations, and observation-driven cloud model outputs. The character of rain events is shown in data samples and summarized in lagged regressions versus surface rain rate. The CAM3 humidity and cloud exhibit little vertical coherence among three distinct layers, and its rain events have a short characteristic time, reflecting the convection scheme?s penetrative nature and its closure?s concentrated sensitivity to a thin boundary layer source level. In contrast, AM2 rain variations have much longer time scales as convection scheme plumes whose entrainment gives them tops below 500 hPa interact with humidity variations in that layer. Plumes detraining at model levels above 500 hPa are restricted by cloud work function thresholds, and upper-tropospheric humidity and cloud layers fed by these are detached from the lower levels and are somewhat sporadic. With these discrete entrainment rates and instability thresholds, AM2 also produces some synthetic-looking noise (sharp features in height and time) on top of its slow rain variations. A distinctive feature of the NASA model is a separate anvil scheme, distinct from the main large-scale cloud scheme, fed by relaxed Arakawa?Schubert (RAS) plume ensemble convection (a different implementation than in AM2). Its variability is rich and vertically coherent, and involves a very strong vertical dipole component to its tropospheric heating variations, of both signs (limited-depth convective heating and top-heavy heating in strong deep events with significant nonconvective rain). Grid-scale saturation events occur in all three models, often without nonconvective surface rain, causing relatively rare episodes of large negative top-of-atmosphere cloud forcing. Overall, cloud forcing regressions show a mild net positive forcing by rain-correlated clouds in CAM3 and mild net cooling in the other models, as the residual of large canceling shortwave and longwave contributions.
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      Virtual Field Campaigns on Deep Tropical Convection in Climate Models

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4208463
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    contributor authorMapes, Brian
    contributor authorBacmeister, Julio
    contributor authorKhairoutdinov, Marat
    contributor authorHannay, Cecile
    contributor authorZhao, Ming
    date accessioned2017-06-09T16:23:37Z
    date available2017-06-09T16:23:37Z
    date copyright2009/01/01
    date issued2009
    identifier issn0894-8755
    identifier otherams-67058.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4208463
    description abstractHigh-resolution time?height data over warm tropical oceans are examined, from three global atmosphere models [GFDL?s Atmosphere Model 2 (AM2), NCAR?s Community Atmosphere Model, version 3 (CAM3), and a NASA Global Modeling and Assimilation Office (GMAO) model], field campaign observations, and observation-driven cloud model outputs. The character of rain events is shown in data samples and summarized in lagged regressions versus surface rain rate. The CAM3 humidity and cloud exhibit little vertical coherence among three distinct layers, and its rain events have a short characteristic time, reflecting the convection scheme?s penetrative nature and its closure?s concentrated sensitivity to a thin boundary layer source level. In contrast, AM2 rain variations have much longer time scales as convection scheme plumes whose entrainment gives them tops below 500 hPa interact with humidity variations in that layer. Plumes detraining at model levels above 500 hPa are restricted by cloud work function thresholds, and upper-tropospheric humidity and cloud layers fed by these are detached from the lower levels and are somewhat sporadic. With these discrete entrainment rates and instability thresholds, AM2 also produces some synthetic-looking noise (sharp features in height and time) on top of its slow rain variations. A distinctive feature of the NASA model is a separate anvil scheme, distinct from the main large-scale cloud scheme, fed by relaxed Arakawa?Schubert (RAS) plume ensemble convection (a different implementation than in AM2). Its variability is rich and vertically coherent, and involves a very strong vertical dipole component to its tropospheric heating variations, of both signs (limited-depth convective heating and top-heavy heating in strong deep events with significant nonconvective rain). Grid-scale saturation events occur in all three models, often without nonconvective surface rain, causing relatively rare episodes of large negative top-of-atmosphere cloud forcing. Overall, cloud forcing regressions show a mild net positive forcing by rain-correlated clouds in CAM3 and mild net cooling in the other models, as the residual of large canceling shortwave and longwave contributions.
    publisherAmerican Meteorological Society
    titleVirtual Field Campaigns on Deep Tropical Convection in Climate Models
    typeJournal Paper
    journal volume22
    journal issue2
    journal titleJournal of Climate
    identifier doi10.1175/2008JCLI2203.1
    journal fristpage244
    journal lastpage257
    treeJournal of Climate:;2009:;volume( 022 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
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