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    The Sea-Breeze Front Analytical Model

    Source: Journal of the Atmospheric Sciences:;1988:;Volume( 045 ):;issue: 006::page 1030
    Author:
    Feliks, Yizhak
    DOI: 10.1175/1520-0469(1988)045<1030:TSBFAM>2.0.CO;2
    Publisher: American Meteorological Society
    Abstract: Analytical solutions to the nonlinear equations of motion are used to describe the sea breeze front. It is found that the front can develop when the atmosphere stratification in the heated layer is neutral or unstable. The temperature drop due to front passage is proportional to the square of the difference between the front speed and the synoptic wind. This square of the difference, on the other hand, is proportional to [2?(s?)/?m]ga where ?(s?) is the mean potential temperature drop across the front and a is the front radius. Fronts which have the same speed of propagation and size, have a larger temperature drop when the synoptic wind blows in the opposite direction to the direction of propagation. Onshore winds associated with strong convergence are obtained in the lower part of the front, while the return current associated with strong divergence is observed in the upper part. The vertical velocity reaches values of some meters per second in the front region. The front propagation is studied in terms of the vorticity equation. The buoyancy term always tends to propagate the front inland. The nonlinear advective term in most of the cases tends to slow this propagation. In some of the cases when buoyancy is very low the advective term tends to propagate the front inland.
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      The Sea-Breeze Front Analytical Model

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4155936
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    contributor authorFeliks, Yizhak
    date accessioned2017-06-09T14:28:08Z
    date available2017-06-09T14:28:08Z
    date copyright1988/03/01
    date issued1988
    identifier issn0022-4928
    identifier otherams-19782.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4155936
    description abstractAnalytical solutions to the nonlinear equations of motion are used to describe the sea breeze front. It is found that the front can develop when the atmosphere stratification in the heated layer is neutral or unstable. The temperature drop due to front passage is proportional to the square of the difference between the front speed and the synoptic wind. This square of the difference, on the other hand, is proportional to [2?(s?)/?m]ga where ?(s?) is the mean potential temperature drop across the front and a is the front radius. Fronts which have the same speed of propagation and size, have a larger temperature drop when the synoptic wind blows in the opposite direction to the direction of propagation. Onshore winds associated with strong convergence are obtained in the lower part of the front, while the return current associated with strong divergence is observed in the upper part. The vertical velocity reaches values of some meters per second in the front region. The front propagation is studied in terms of the vorticity equation. The buoyancy term always tends to propagate the front inland. The nonlinear advective term in most of the cases tends to slow this propagation. In some of the cases when buoyancy is very low the advective term tends to propagate the front inland.
    publisherAmerican Meteorological Society
    titleThe Sea-Breeze Front Analytical Model
    typeJournal Paper
    journal volume45
    journal issue6
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/1520-0469(1988)045<1030:TSBFAM>2.0.CO;2
    journal fristpage1030
    journal lastpage1038
    treeJournal of the Atmospheric Sciences:;1988:;Volume( 045 ):;issue: 006
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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