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    Simulation of a Stratocumulus-Topped Planetary Boundary Layer: Intercomparison among Different Numerical Codes

    Source: Bulletin of the American Meteorological Society:;1996:;volume( 077 ):;issue: 002::page 261
    Author:
    Moeng, C-H.
    ,
    Cotton, W. R.
    ,
    Stevens, B.
    ,
    Bretherton, C.
    ,
    Rand, H. A.
    ,
    Chlond, A.
    ,
    Khairoutdinov, M.
    ,
    Krueger, S.
    ,
    Lewellen, W. S.
    ,
    MacVean, M. K.
    ,
    Pasquier, J. R. M.
    ,
    Siebesma, A. P.
    ,
    Sykes, R. I.
    DOI: 10.1175/1520-0477(1996)077<0261:SOASTP>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: This paper reports an intercomparison study of a stratocumulus-topped planetary boundary layer (PBL) generated from ten 3D large eddy simulation (LES) codes and four 2D cloud-resolving models (CRMs). These models vary in the numerics, the parameterizations of the subgrid-scale (SGS) turbulence and condensation processes, and the calculation of longwave radiative cooling. Cloud-top radiative cooling is often the major source of buoyant production of turbulent kinetic energy in the stratocumulus-topped PBL. An idealized nocturnal stratocumulus case was selected for this study. It featured a statistically horizontally homogeneous and nearly solid cloud deck with no drizzle, no solar radiation, little wind shear, and little surface heating. Results of the two-hour simulations showed that the overall cloud structure, including cloud-top height, cloud fraction, and the vertical distributions of many turbulence statistics, compared well among all LESs despite the code variations. However, the entrainment rate was found to differ significantly among the simulations. Among the model uncertainties due to numerics, SGS turbulence, SGS condensation, and radiation, none could be identified to explain such differences. Therefore, a follow-up study will focus on simulating the entrainment process. The liquid water mixing ratio profiles also varied significantly among the simulators; these profiles are sensitive to the algorithm used for computing the saturation mixing ratio. Despite the obvious differences in eddy structure in two- and three-dimensional simulations, the cloud structure predicted by the 2D CRMs was similar to that obtained by the 3D LESs, even though the momentum fluxes, the vertical and horizontal velocity valances, and the turbulence kinetic energy profiles predicted by the 2D CRMs all differ significantly from those of the LESs.
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      Simulation of a Stratocumulus-Topped Planetary Boundary Layer: Intercomparison among Different Numerical Codes

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4161319
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    contributor authorMoeng, C-H.
    contributor authorCotton, W. R.
    contributor authorStevens, B.
    contributor authorBretherton, C.
    contributor authorRand, H. A.
    contributor authorChlond, A.
    contributor authorKhairoutdinov, M.
    contributor authorKrueger, S.
    contributor authorLewellen, W. S.
    contributor authorMacVean, M. K.
    contributor authorPasquier, J. R. M.
    contributor authorSiebesma, A. P.
    contributor authorSykes, R. I.
    date accessioned2017-06-09T14:41:40Z
    date available2017-06-09T14:41:40Z
    date copyright1996/02/01
    date issued1996
    identifier issn0003-0007
    identifier otherams-24626.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4161319
    description abstractThis paper reports an intercomparison study of a stratocumulus-topped planetary boundary layer (PBL) generated from ten 3D large eddy simulation (LES) codes and four 2D cloud-resolving models (CRMs). These models vary in the numerics, the parameterizations of the subgrid-scale (SGS) turbulence and condensation processes, and the calculation of longwave radiative cooling. Cloud-top radiative cooling is often the major source of buoyant production of turbulent kinetic energy in the stratocumulus-topped PBL. An idealized nocturnal stratocumulus case was selected for this study. It featured a statistically horizontally homogeneous and nearly solid cloud deck with no drizzle, no solar radiation, little wind shear, and little surface heating. Results of the two-hour simulations showed that the overall cloud structure, including cloud-top height, cloud fraction, and the vertical distributions of many turbulence statistics, compared well among all LESs despite the code variations. However, the entrainment rate was found to differ significantly among the simulations. Among the model uncertainties due to numerics, SGS turbulence, SGS condensation, and radiation, none could be identified to explain such differences. Therefore, a follow-up study will focus on simulating the entrainment process. The liquid water mixing ratio profiles also varied significantly among the simulators; these profiles are sensitive to the algorithm used for computing the saturation mixing ratio. Despite the obvious differences in eddy structure in two- and three-dimensional simulations, the cloud structure predicted by the 2D CRMs was similar to that obtained by the 3D LESs, even though the momentum fluxes, the vertical and horizontal velocity valances, and the turbulence kinetic energy profiles predicted by the 2D CRMs all differ significantly from those of the LESs.
    publisherAmerican Meteorological Society
    titleSimulation of a Stratocumulus-Topped Planetary Boundary Layer: Intercomparison among Different Numerical Codes
    typeJournal Paper
    journal volume77
    journal issue2
    journal titleBulletin of the American Meteorological Society
    identifier doi10.1175/1520-0477(1996)077<0261:SOASTP>2.0.CO;2
    journal fristpage261
    journal lastpage278
    treeBulletin of the American Meteorological Society:;1996:;volume( 077 ):;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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