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首页> 外文期刊>Journal of Physical Oceanography >Near-Surface Turbulence in the Presence of Breaking Waves
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Near-Surface Turbulence in the Presence of Breaking Waves

机译:破碎波作用下的近地表湍流

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Observations with a three-axis pulse-to-pulse coherent acoustic Doppler profiler and acoustic resonators reveal the turbulence and bubble field beneath breaking waves in the open ocean at wind speeds up to 14 m s~(-1). About 55%-80% of velocity wavenumber spectra, calculated with Hilbert spectral analysis based on empirical mode decomposition, are consistent with an inertial subrange. Time series of turbulent kinetic energy dissipation at approximately 1 m beneath the free surface and 1-Hz sampling rate are obtained. High turbulence levels with dissipation rates more than four orders larger than the background dissipation are linked to wave breaking. Initial dissipation levels beneath breaking waves yield the Hinze scale of the maximum bubble size a_H ≈ 2 X 10 ~(-3) m. Turbulence induced by discrete breaking events was observed to decay as ε ∝ t~n, where n = -4.3 is close to the theoretical value for isotropic turbulence ( ― 17/4). In the crest region above the mean waterline, dissipation increases as ε(z) ∝ z~(2.3). Depth-integrated dissipation in the crest region is more than 2 times the depth-integrated dissipation in the trough region. Adjusting the surface definition in common turbulence models to reflect the observed dissipation profile improves the agreement between modeled and observed dissipation. There is some evidence that turbulent dissipation increases above the background level prior to the air entrainment. The magnitude and occurrence of the prebreaking turbulence are consistent with wave- turbulence interaction in a rotational wave field.
机译:用三轴脉冲至脉冲相干声多普勒剖面仪和声谐振器进行的观测揭示了在风速高达14 m s〜(-1)的大洋中,破碎波下方的湍流和气泡场。通过基于经验模态分解的希尔伯特频谱分析计算得出的速度波数频谱的大约55%-80%与惯性子范围一致。获得了在自由表面以下约1 m处湍流动能耗散和1-Hz采样率的时间序列。耗散率比背景耗散大四倍以上的高湍流水平与断波有关。破碎波下的初始耗散水平产生最大气泡尺寸a_H≈2 X 10〜(-3)m的Hinze尺度。观察到由离散破裂事件引起的湍流随着ε∝ t〜n衰减,其中n = -4.3接近于各向同性湍流的理论值(〜17/4)。在平均水线以上的波峰区域,耗散随着ε(z)∝ z〜(2.3)的增加而增加。波峰区域的深度积分耗散是波谷区域的深度积分耗散的2倍以上。调整常见湍流模型中的表面清晰度以反映观察到的耗散曲线可以改善建模耗散与观察到的耗散之间的一致性。有证据表明,在夹带空气之前,湍流耗散增加到背景水平以上。爆发湍流的大小和发生与旋转波场中的湍流相互作用是一致的。

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