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    Alternative Nonlocal Descriptions of Boundary-Layer Evolution

    Source: Journal of the Atmospheric Sciences:;1992:;Volume( 049 ):;issue: 023::page 2267
    Author:
    Zhang, Qing
    ,
    Stull, Roland
    DOI: 10.1175/1520-0469(1992)049<2267:ANDOBL>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Two alternative parameterizations for nonlocal turbulence mixing are tested in a 1D boundary-layer model against a dataset from the 1983 Boundary-Layer Experiment (BLX83) in Oklahoma. One method, proposed previously by Stull and Driedonks, is based on a nonlocal approximation to the turbulence kinetic energy (TKE) equation. An alternate method, based on a nonlocal approximation to the Richardson number, is simplified here from earlier parameterizations for transilient turbulence theory. Convective mixed-layer simulations of the vertical profiles of mean variables and fluxes using both methods are compared to the BLX83 observations and to simulations using a traditional slab model. The TKE method develops a surface layer that is too thick compared to BLX83 data, particularly in the early morning. It also lacks the subadiabatic lapse rate that is observed in the top of the mixed layer. The Richardson number approach produces more accurate mixed-layer profiles, but lacks the general physical interpretation of the TKE method. Nonlocal spectral decompositions of the flux and intensity of mixing confirm that large-size eddies dominate within the middle of the mixed layer. Based on this limited validation, the Richardson number method is recommended for convective boundary layers, but the TKE approach should be used for modeling more general boundary layers that can include clouds and stable and/or windy conditions.
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      Alternative Nonlocal Descriptions of Boundary-Layer Evolution

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    contributor authorZhang, Qing
    contributor authorStull, Roland
    date accessioned2017-06-09T14:31:08Z
    date available2017-06-09T14:31:08Z
    date copyright1992/12/01
    date issued1992
    identifier issn0022-4928
    identifier otherams-20795.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4157062
    description abstractTwo alternative parameterizations for nonlocal turbulence mixing are tested in a 1D boundary-layer model against a dataset from the 1983 Boundary-Layer Experiment (BLX83) in Oklahoma. One method, proposed previously by Stull and Driedonks, is based on a nonlocal approximation to the turbulence kinetic energy (TKE) equation. An alternate method, based on a nonlocal approximation to the Richardson number, is simplified here from earlier parameterizations for transilient turbulence theory. Convective mixed-layer simulations of the vertical profiles of mean variables and fluxes using both methods are compared to the BLX83 observations and to simulations using a traditional slab model. The TKE method develops a surface layer that is too thick compared to BLX83 data, particularly in the early morning. It also lacks the subadiabatic lapse rate that is observed in the top of the mixed layer. The Richardson number approach produces more accurate mixed-layer profiles, but lacks the general physical interpretation of the TKE method. Nonlocal spectral decompositions of the flux and intensity of mixing confirm that large-size eddies dominate within the middle of the mixed layer. Based on this limited validation, the Richardson number method is recommended for convective boundary layers, but the TKE approach should be used for modeling more general boundary layers that can include clouds and stable and/or windy conditions.
    publisherAmerican Meteorological Society
    titleAlternative Nonlocal Descriptions of Boundary-Layer Evolution
    typeJournal Paper
    journal volume49
    journal issue23
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1992)049<2267:ANDOBL>2.0.CO;2
    journal fristpage2267
    journal lastpage2281
    treeJournal of the Atmospheric Sciences:;1992:;Volume( 049 ):;issue: 023
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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