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    Shoreline Profile of Stokes‐Mode Edge Waves

    Source: Journal of Waterway, Port, Coastal, and Ocean Engineering:;1992:;Volume ( 118 ):;issue: 001
    Author:
    Harry H. Yeh
    DOI: 10.1061/(ASCE)0733-950X(1992)118:1(112)
    Publisher: American Society of Civil Engineers
    Abstract: Stokes-mode edge waves in an inviscid-fluid and irrotational-flow domain have simmlar characteristics as deep-water waves. The mathematical presentations of edge waves are identical, except the coefficients, to those of deep-water waves when the coordinate axes are rotated so that one of the axes points along the beach surface in the offshore direction. Although the similarities appear to exist in their nonlinear wave solutions, the second-harmonic component on the runup wave profile of edge waves arises from the first higher-order solution whereas, in deep-water waves, such a characteristic appears in the second higher-order solution. This early appearance of the nonlinear effect in the runup profile is due to the flow restriction caused by the beach geometry. On the other hand, the vertical water-surface displacement of edge waves has no second-harmonic component at the first-order solution, instead has the characteristic of the set-down of mean water level.
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      Shoreline Profile of Stokes‐Mode Edge Waves

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    http://yetl.yabesh.ir/yetl1/handle/yetl/40916
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    • Journal of Waterway, Port, Coastal, and Ocean Engineering

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    contributor authorHarry H. Yeh
    date accessioned2017-05-08T21:09:33Z
    date available2017-05-08T21:09:33Z
    date copyrightJanuary 1992
    date issued1992
    identifier other%28asce%290733-950x%281992%29118%3A1%28112%29.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/40916
    description abstractStokes-mode edge waves in an inviscid-fluid and irrotational-flow domain have simmlar characteristics as deep-water waves. The mathematical presentations of edge waves are identical, except the coefficients, to those of deep-water waves when the coordinate axes are rotated so that one of the axes points along the beach surface in the offshore direction. Although the similarities appear to exist in their nonlinear wave solutions, the second-harmonic component on the runup wave profile of edge waves arises from the first higher-order solution whereas, in deep-water waves, such a characteristic appears in the second higher-order solution. This early appearance of the nonlinear effect in the runup profile is due to the flow restriction caused by the beach geometry. On the other hand, the vertical water-surface displacement of edge waves has no second-harmonic component at the first-order solution, instead has the characteristic of the set-down of mean water level.
    publisherAmerican Society of Civil Engineers
    titleShoreline Profile of Stokes‐Mode Edge Waves
    typeJournal Paper
    journal volume118
    journal issue1
    journal titleJournal of Waterway, Port, Coastal, and Ocean Engineering
    identifier doi10.1061/(ASCE)0733-950X(1992)118:1(112)
    treeJournal of Waterway, Port, Coastal, and Ocean Engineering:;1992:;Volume ( 118 ):;issue: 001
    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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