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    Potential Vorticity Inversion on a Hemisphere

    Source: Journal of the Atmospheric Sciences:;2000:;Volume( 057 ):;issue: 009::page 1214
    Author:
    McIntyre, Michael E.
    ,
    Norton, Warwick A.
    DOI: 10.1175/1520-0469(2000)057<1214:PVIOAH>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Several different kinds of accurate potential vorticity (PV) inversion operators, and the associated balanced models, are tested for the shallow water equations on a hemisphere in an attempt to approach the ultimate limitations of the balance, inversion, and slow-manifold concepts. The accuracies achieved are far higher than for standard balanced models accurate to one or two orders in Rossby number R or Froude number F (where F = |u|/c; |u| = flow speed; and c = gravity wave speed). Numerical inversions, and corresponding balanced-model integrations testing cumulative accuracy, are carried out for cases that include substantial PV anomalies in the Tropics. The balanced models in question are constructed so as to be exactly PV conserving and to have unique velocity fields (implying, incidentally, that they cannot be Hamiltonian). Mean layer depths of 1 and 2 km are tested. The results show that, in the cases studied, the dynamical information contained in PV distributions is remarkably close to being complete even though R = ∞ at the equator and even though local maximum Froude numbers, Fmax, approach unity in some cases. For example, in a 10-day integration of the balanced model corresponding to one of the most accurate inversion operators, ?third-order normal mode inversion,? the mean depth was 1 km, the minimum depth less than 0.5 km, and Fmax ? 0.7, hardly small in comparison with unity. At the end of 10 days of integration, the cumulative rms error in the layer depth was less than 15 m, that is, less than 5% of the typical rms spatial variation of 310 m. At the end of the first day of integration the rms error was 5 m, that is, less than 2%. Here ?error? refers to a comparison between the results of a balanced integration and those of a corresponding primitive equation integration initialized to have low gravity wave activity on day 0. Contour maps of the PV distributions remained almost indistinguishable by eye over the 10-day period. This remarkable cumulative accuracy, far beyond anything that could have been expected from standard scale analysis, is probably related to the weakness of the spontaneous-adjustment emission or ?Lighthill radiation? studied in the companion paper by Ford et al
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      Potential Vorticity Inversion on a Hemisphere

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    contributor authorMcIntyre, Michael E.
    contributor authorNorton, Warwick A.
    date accessioned2017-06-09T14:36:06Z
    date available2017-06-09T14:36:06Z
    date copyright2000/05/01
    date issued2000
    identifier issn0022-4928
    identifier otherams-22587.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4159053
    description abstractSeveral different kinds of accurate potential vorticity (PV) inversion operators, and the associated balanced models, are tested for the shallow water equations on a hemisphere in an attempt to approach the ultimate limitations of the balance, inversion, and slow-manifold concepts. The accuracies achieved are far higher than for standard balanced models accurate to one or two orders in Rossby number R or Froude number F (where F = |u|/c; |u| = flow speed; and c = gravity wave speed). Numerical inversions, and corresponding balanced-model integrations testing cumulative accuracy, are carried out for cases that include substantial PV anomalies in the Tropics. The balanced models in question are constructed so as to be exactly PV conserving and to have unique velocity fields (implying, incidentally, that they cannot be Hamiltonian). Mean layer depths of 1 and 2 km are tested. The results show that, in the cases studied, the dynamical information contained in PV distributions is remarkably close to being complete even though R = ∞ at the equator and even though local maximum Froude numbers, Fmax, approach unity in some cases. For example, in a 10-day integration of the balanced model corresponding to one of the most accurate inversion operators, ?third-order normal mode inversion,? the mean depth was 1 km, the minimum depth less than 0.5 km, and Fmax ? 0.7, hardly small in comparison with unity. At the end of 10 days of integration, the cumulative rms error in the layer depth was less than 15 m, that is, less than 5% of the typical rms spatial variation of 310 m. At the end of the first day of integration the rms error was 5 m, that is, less than 2%. Here ?error? refers to a comparison between the results of a balanced integration and those of a corresponding primitive equation integration initialized to have low gravity wave activity on day 0. Contour maps of the PV distributions remained almost indistinguishable by eye over the 10-day period. This remarkable cumulative accuracy, far beyond anything that could have been expected from standard scale analysis, is probably related to the weakness of the spontaneous-adjustment emission or ?Lighthill radiation? studied in the companion paper by Ford et al
    publisherAmerican Meteorological Society
    titlePotential Vorticity Inversion on a Hemisphere
    typeJournal Paper
    journal volume57
    journal issue9
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(2000)057<1214:PVIOAH>2.0.CO;2
    journal fristpage1214
    journal lastpage1235
    treeJournal of the Atmospheric Sciences:;2000:;Volume( 057 ):;issue: 009
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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