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    Nonlinear Infragravity–Wave Interactions on a Gently Sloping Laboratory Beach

    Source: Journal of Physical Oceanography:;2014:;Volume( 045 ):;issue: 002::page 589
    Author:
    de Bakker, A. T. M.
    ,
    Herbers, T. H. C.
    ,
    Smit, P. B.
    ,
    Tissier, M. F. S.
    ,
    Ruessink, B. G.
    DOI: 10.1175/JPO-D-14-0186.1
    Publisher: American Meteorological Society
    Abstract: high-resolution dataset of three irregular wave conditions collected on a gently sloping laboratory beach is analyzed to study nonlinear energy transfers involving infragravity frequencies. This study uses bispectral analysis to identify the dominant, nonlinear interactions and estimate energy transfers to investigate energy flows within the spectra. Energy flows are identified by dividing transfers into four types of triad interactions, with triads including one, two, or three infragravity?frequency components, and triad interactions solely between short-wave frequencies. In the shoaling zone, the energy transfers are generally from the spectral peak to its higher harmonics and to infragravity frequencies. While receiving net energy, infragravity waves participate in interactions that spread energy of the short-wave peaks to adjacent frequencies, thereby creating a broader energy spectrum. In the short-wave surf zone, infragravity?infragravity interactions develop, and close to shore, they dominate the interactions. Nonlinear energy fluxes are compared to gradients in total energy flux and are observed to balance nearly completely. Overall, energy losses at both infragravity and short-wave frequencies can largely be explained by a cascade of nonlinear energy transfers to high frequencies (say, f > 1.5 Hz) where the energy is presumably dissipated. Infragravity?infragravity interactions seem to induce higher harmonics that allow for shape transformation of the infragravity wave to asymmetric. The largest decrease in infragravity wave height occurs close to the shore, where infragravity?infragravity interactions dominate and where the infragravity wave is asymmetric, suggesting wave breaking to be the dominant mechanism of infragravity wave dissipation.
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      Nonlinear Infragravity–Wave Interactions on a Gently Sloping Laboratory Beach

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    http://yetl.yabesh.ir/yetl1/handle/yetl/4226906
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    contributor authorde Bakker, A. T. M.
    contributor authorHerbers, T. H. C.
    contributor authorSmit, P. B.
    contributor authorTissier, M. F. S.
    contributor authorRuessink, B. G.
    date accessioned2017-06-09T17:21:06Z
    date available2017-06-09T17:21:06Z
    date copyright2015/02/01
    date issued2014
    identifier issn0022-3670
    identifier otherams-83657.pdf
    identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4226906
    description abstracthigh-resolution dataset of three irregular wave conditions collected on a gently sloping laboratory beach is analyzed to study nonlinear energy transfers involving infragravity frequencies. This study uses bispectral analysis to identify the dominant, nonlinear interactions and estimate energy transfers to investigate energy flows within the spectra. Energy flows are identified by dividing transfers into four types of triad interactions, with triads including one, two, or three infragravity?frequency components, and triad interactions solely between short-wave frequencies. In the shoaling zone, the energy transfers are generally from the spectral peak to its higher harmonics and to infragravity frequencies. While receiving net energy, infragravity waves participate in interactions that spread energy of the short-wave peaks to adjacent frequencies, thereby creating a broader energy spectrum. In the short-wave surf zone, infragravity?infragravity interactions develop, and close to shore, they dominate the interactions. Nonlinear energy fluxes are compared to gradients in total energy flux and are observed to balance nearly completely. Overall, energy losses at both infragravity and short-wave frequencies can largely be explained by a cascade of nonlinear energy transfers to high frequencies (say, f > 1.5 Hz) where the energy is presumably dissipated. Infragravity?infragravity interactions seem to induce higher harmonics that allow for shape transformation of the infragravity wave to asymmetric. The largest decrease in infragravity wave height occurs close to the shore, where infragravity?infragravity interactions dominate and where the infragravity wave is asymmetric, suggesting wave breaking to be the dominant mechanism of infragravity wave dissipation.
    publisherAmerican Meteorological Society
    titleNonlinear Infragravity–Wave Interactions on a Gently Sloping Laboratory Beach
    typeJournal Paper
    journal volume45
    journal issue2
    journal titleJournal of Physical Oceanography
    identifier doi10.1175/JPO-D-14-0186.1
    journal fristpage589
    journal lastpage605
    treeJournal of Physical Oceanography:;2014:;Volume( 045 ):;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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