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首页> 外文期刊>Journal of Geophysical Research, C. Oceans: JGR >Bubbles generated from wind-steepened breaking waves: 2. Bubble plumes, bubbles, and wave characteristics
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Bubbles generated from wind-steepened breaking waves: 2. Bubble plumes, bubbles, and wave characteristics

机译:风速增强的碎波产生的气泡:2.气泡羽,气泡和波浪特征

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摘要

Measurements of breaking-wave-generated bubble plumes were made in fresh (but not clean) water in a large wind-wave tunnel. To preserve diversity, a classification scheme was developed on the basis of plume dimensions and “optical density,” or the plume's ability to obscure the background. Optically dense plumes were due to the presence of a peak at large radius in the plume bubble size distribution. For each class, the plume formation rate, P, was measured at different fetches. The relationship between wave-breaking characteristics and the bubble plume evolution is examined in detail for these experiments. The wave-breaking rate and intensity were strongly fetch-dependent as the mechanically steepened wind waves rapidly evolved with fetch because of wind, dissipation, and nonlinear wave-wave interactions. P followed the trend in wave breaking, reaching a maximum at the fetch of maximum wave breaking. The ratio of dense to diffuse plumes was more sensitive to the wave-breaking intensity. Using P and the bubble population size distributions for each class, the global bubble plume injection size distribution, Ψi(r), where r is radius, was calculated. Ψi decreased as Ψi ~ r ?1.2 for r < 1700 μm and Ψi ~ r ?3.9 for larger r. Total volume injection was 640 cm3 s?1, divided approximately equally between bubbles smaller and larger than 1700-μm radius. Using plume volumes at maximum penetration for each class, a concentration distribution was calculated and showed plume concentrations greater than the background population by one to several orders of magnitude, depending upon r.
机译:破波产生的气泡羽流的测量是在大型风波隧道中的淡水(但不是干净的)中进行的。为了保持多样性,在烟羽尺寸和“光学密度”或烟羽掩盖背景的能力的基础上,开发了一种分类方案。光学上密集的羽流是由于羽流气泡尺寸分布中的大半径处存在峰值所致。对于每个类别,在不同读取时测量羽流形成率P。对于这些实验,详细检查了波浪破碎特性与气泡羽流演变之间的关系。由于受风,耗散和非线性波-波相互作用的影响,机械陡峭的风波随取而快速演化,因此破波速率和强度强烈依赖于取波。 P遵循波浪破碎的趋势,在获取最大波浪破碎时达到最大值。密集羽流与弥散羽流的比率对波强度更敏感。使用P和每个类别的气泡总体大小分布,可以计算出总体气泡羽状喷射尺寸分布Ψi(r),其中r是半径。 r <1700μm时,Ψi减小为Ψi〜r?1.2,较大r时,Ψi〜r?3.9。总注入量为640 cm3 s?1,在小于和大于1700-μm半径的气泡之间平均分配。使用每种类别在最大渗透量下的羽流体积,计算浓度分布,并显示羽流浓度比背景种群大一到几个数量级,具体取决于r。

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