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    What Are the Sources of Mechanical Damping in Matsuno–Gill-Type Models?

    Source: Journal of Climate:;2008:;volume( 021 ):;issue: 002::page 165
    Author:
    Lin, Jia-Lin
    ,
    Mapes, Brian E.
    ,
    Han, Weiqing
    DOI: 10.1175/2007JCLI1546.1
    Publisher: American Meteorological Society
    Abstract: The Matsuno?Gill model has been widely used to study the tropical large-scale circulations and atmosphere?ocean interactions. However, a common critique of this model is that it requires a strong equivalent linear mechanical damping to get realistic wind response and it is unclear what could provide such a strong damping above the boundary layer. This study evaluates the sources and strength of equivalent linear mechanical damping in the Walker circulation by calculating the zonal momentum budget using 15 yr (1979?93) of daily global reanalysis data. Two different reanalyses [NCEP?NCAR and 15-yr ECMWF Re-Analysis (ERA-15)] give qualitatively similar results for all major terms, including the budget residual, whose structure is consistent with its interpretation as eddy momentum flux convergence by convective momentum transport (CMT). The Walker circulation is characterized by two distinct regions: a deep convection region over the Indo-Pacific warm pool and a shallow convection region over the eastern Pacific cold tongue. These two regions are separated by a strong upper-tropospheric ridge and a strong lower-tropospheric trough in the central Pacific. The resultant pressure gradient forces on both sides require strong (approximately 5?10 days) damping to balance them because Coriolis force near the equator is too small to provide the balance. In the deep convection region, the damping is provided by CMT and advection together in both the upper and lower troposphere. In the shallow convection region, on the other hand, the damping is provided mainly by advection in the upper troposphere and by CMT in the lower troposphere. In other words, the upper-level tropical easterly jet and the low-level trade wind are both braked by CMT. These results support the use of strong damping in the Matsuno?Gill-type models but suggest that the damping rate is spatially inhomogeneous and the CMT-related damping increases with the strength of convection. Implications for GCM?s simulation of tropical mean climate are discussed.
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      What Are the Sources of Mechanical Damping in Matsuno–Gill-Type Models?

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4206915
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    contributor authorLin, Jia-Lin
    contributor authorMapes, Brian E.
    contributor authorHan, Weiqing
    date accessioned2017-06-09T16:19:10Z
    date available2017-06-09T16:19:10Z
    date copyright2008/01/01
    date issued2008
    identifier issn0894-8755
    identifier otherams-65665.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4206915
    description abstractThe Matsuno?Gill model has been widely used to study the tropical large-scale circulations and atmosphere?ocean interactions. However, a common critique of this model is that it requires a strong equivalent linear mechanical damping to get realistic wind response and it is unclear what could provide such a strong damping above the boundary layer. This study evaluates the sources and strength of equivalent linear mechanical damping in the Walker circulation by calculating the zonal momentum budget using 15 yr (1979?93) of daily global reanalysis data. Two different reanalyses [NCEP?NCAR and 15-yr ECMWF Re-Analysis (ERA-15)] give qualitatively similar results for all major terms, including the budget residual, whose structure is consistent with its interpretation as eddy momentum flux convergence by convective momentum transport (CMT). The Walker circulation is characterized by two distinct regions: a deep convection region over the Indo-Pacific warm pool and a shallow convection region over the eastern Pacific cold tongue. These two regions are separated by a strong upper-tropospheric ridge and a strong lower-tropospheric trough in the central Pacific. The resultant pressure gradient forces on both sides require strong (approximately 5?10 days) damping to balance them because Coriolis force near the equator is too small to provide the balance. In the deep convection region, the damping is provided by CMT and advection together in both the upper and lower troposphere. In the shallow convection region, on the other hand, the damping is provided mainly by advection in the upper troposphere and by CMT in the lower troposphere. In other words, the upper-level tropical easterly jet and the low-level trade wind are both braked by CMT. These results support the use of strong damping in the Matsuno?Gill-type models but suggest that the damping rate is spatially inhomogeneous and the CMT-related damping increases with the strength of convection. Implications for GCM?s simulation of tropical mean climate are discussed.
    publisherAmerican Meteorological Society
    titleWhat Are the Sources of Mechanical Damping in Matsuno–Gill-Type Models?
    typeJournal Paper
    journal volume21
    journal issue2
    journal titleJournal of Climate
    identifier doi10.1175/2007JCLI1546.1
    journal fristpage165
    journal lastpage179
    treeJournal of Climate:;2008:;volume( 021 ):;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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