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    Effect of Swell on Wind Stress for Light to Moderate Winds

    Source: Journal of the Atmospheric Sciences:;2020:;volume( 77 ):;issue: 011::page 3759
    Author:
    Vincent, Charles L.;Graber, Hans C.;Collins, Clarence O., III
    DOI: 10.1175/JAS-D-19-0338.1
    Publisher: American Meteorological Society
    Abstract: Buoy observations from a 1999 Gulf of Mexico field program (GOM99) are used to investigate the relationships among friction velocity u*, wind speed U, and amount of swell present. A U–u*sea parameterization is developed for the case of pure wind sea (denoted by u*sea), which is linear in U over the range of available winds (2–16 m s−1). The curve shows no sign of an inflection point near 7–8 m s−1 as suggested in a 2012 paper by Andreas et al. on the basis of a transition from smooth to rough flow. When observations containing more than minimal swell energy are included, a different U–u* equation for U < 8 m s−1 is found, which would intersect the pure wind-sea curve about 7–8 m s−1. These two relationships yield a bilinear curve similar to Andreas et al. with an apparent inflection near 7–8 m s−1. The absence of the inflection in the GOM99 experiment pure wind-sea curve and the similarity of the GOM99 swell-dominated low wind speed to Andreas et al.’s low wind speed relationship suggest that the inflection may be due to the effect of swell and not a flow transition. Swell heights in the range of only 25–50 cm may be sufficient to impact stress at low wind speeds.
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      Effect of Swell on Wind Stress for Light to Moderate Winds

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    contributor authorVincent, Charles L.;Graber, Hans C.;Collins, Clarence O., III
    date accessioned2022-01-30T17:50:49Z
    date available2022-01-30T17:50:49Z
    date copyright10/20/2020 12:00:00 AM
    date issued2020
    identifier issn0022-4928
    identifier otherjasd190338.pdf
    identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4264041
    description abstractBuoy observations from a 1999 Gulf of Mexico field program (GOM99) are used to investigate the relationships among friction velocity u*, wind speed U, and amount of swell present. A U–u*sea parameterization is developed for the case of pure wind sea (denoted by u*sea), which is linear in U over the range of available winds (2–16 m s−1). The curve shows no sign of an inflection point near 7–8 m s−1 as suggested in a 2012 paper by Andreas et al. on the basis of a transition from smooth to rough flow. When observations containing more than minimal swell energy are included, a different U–u* equation for U < 8 m s−1 is found, which would intersect the pure wind-sea curve about 7–8 m s−1. These two relationships yield a bilinear curve similar to Andreas et al. with an apparent inflection near 7–8 m s−1. The absence of the inflection in the GOM99 experiment pure wind-sea curve and the similarity of the GOM99 swell-dominated low wind speed to Andreas et al.’s low wind speed relationship suggest that the inflection may be due to the effect of swell and not a flow transition. Swell heights in the range of only 25–50 cm may be sufficient to impact stress at low wind speeds.
    publisherAmerican Meteorological Society
    titleEffect of Swell on Wind Stress for Light to Moderate Winds
    typeJournal Paper
    journal volume77
    journal issue11
    journal titleJournal of the Atmospheric Sciences
    identifier doi10.1175/JAS-D-19-0338.1
    journal fristpage3759
    journal lastpage3768
    treeJournal of the Atmospheric Sciences:;2020:;volume( 77 ):;issue: 011
    contenttypeFulltext
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