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    A Comparison of Quasigeostrophic and Nonquasigeostrophic Vertical Motions for a Model-simulated Rapidly Intensifying Marine Extratropical Cyclone

    Source: Monthly Weather Review:;1992:;volume( 120 ):;issue: 007::page 1108
    Author:
    Pauley, Patricia M.
    ,
    Nieman, Steven J.
    DOI: 10.1175/1520-0493(1992)120<1108:ACOQAN>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Large-scale departures from quasigeostrophic vertical motions are diagnosed for a model simulation of the QE II storm (9?11 September 1978). The simulation was performed by the Limited-Area Mesoscale Prediction System (LAMPS), initialized at 1200 UTC 9 September 1978. The model cyclone intensified from a central pressure of 1003 mb to 976 mb in 24 h, considerably short of the 59 mb (24 h)?1 observed deepening but reasonable in comparison to other model simulations of this storm. This diagnosis centers on a hydrostatic generalized omega equation, which scales to the quasigeostiophic omega equation for small Rossby number. Vertical motions were computed both from this generalized omega equation and the quasigeostrophic omega equation in order to examine the importance of nonquasigeostrophic effects. The high correlation of vertical motions from a control experiment (using most of the terms in the generalized omega equation) with the vertical motions predicted by the model establishes the validity of the method. A further comparison against satellite imagery also shows that these computed vertical motions portray a pattern similar to the satellite cloud shield. However, the pattern and magnitude of the quasigeostrophic vertical motions are quite different from those of the generalized vertical motions. An evaluation of individual terms in the generalized equation shows that although additional terms in omega placed on the left-hand side significantly affect the magnitude of the vertical motion, the greatest nonquasigeostrophic effects are provided by the diabatic term and the ageostrophic advections. Latent heating greatly enhances the upward motion in the cyclone?s cloud shield, while ageostrophic advections both suppress downward motion behind the cold front and enhance upward motion near the warm front.
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      A Comparison of Quasigeostrophic and Nonquasigeostrophic Vertical Motions for a Model-simulated Rapidly Intensifying Marine Extratropical Cyclone

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4202802
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    • Monthly Weather Review

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    contributor authorPauley, Patricia M.
    contributor authorNieman, Steven J.
    date accessioned2017-06-09T16:08:46Z
    date available2017-06-09T16:08:46Z
    date copyright1992/07/01
    date issued1992
    identifier issn0027-0644
    identifier otherams-61963.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4202802
    description abstractLarge-scale departures from quasigeostrophic vertical motions are diagnosed for a model simulation of the QE II storm (9?11 September 1978). The simulation was performed by the Limited-Area Mesoscale Prediction System (LAMPS), initialized at 1200 UTC 9 September 1978. The model cyclone intensified from a central pressure of 1003 mb to 976 mb in 24 h, considerably short of the 59 mb (24 h)?1 observed deepening but reasonable in comparison to other model simulations of this storm. This diagnosis centers on a hydrostatic generalized omega equation, which scales to the quasigeostiophic omega equation for small Rossby number. Vertical motions were computed both from this generalized omega equation and the quasigeostrophic omega equation in order to examine the importance of nonquasigeostrophic effects. The high correlation of vertical motions from a control experiment (using most of the terms in the generalized omega equation) with the vertical motions predicted by the model establishes the validity of the method. A further comparison against satellite imagery also shows that these computed vertical motions portray a pattern similar to the satellite cloud shield. However, the pattern and magnitude of the quasigeostrophic vertical motions are quite different from those of the generalized vertical motions. An evaluation of individual terms in the generalized equation shows that although additional terms in omega placed on the left-hand side significantly affect the magnitude of the vertical motion, the greatest nonquasigeostrophic effects are provided by the diabatic term and the ageostrophic advections. Latent heating greatly enhances the upward motion in the cyclone?s cloud shield, while ageostrophic advections both suppress downward motion behind the cold front and enhance upward motion near the warm front.
    publisherAmerican Meteorological Society
    titleA Comparison of Quasigeostrophic and Nonquasigeostrophic Vertical Motions for a Model-simulated Rapidly Intensifying Marine Extratropical Cyclone
    typeJournal Paper
    journal volume120
    journal issue7
    journal titleMonthly Weather Review
    identifier doi10.1175/1520-0493(1992)120<1108:ACOQAN>2.0.CO;2
    journal fristpage1108
    journal lastpage1134
    treeMonthly Weather Review:;1992:;volume( 120 ):;issue: 007
    contenttypeFulltext
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