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arXiv 2411.03415physics.flu-dyn
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风驱破碎波中的动量通量

Momentum fluxes in wind-forced breaking waves

Nicolò Scapin, Jiarong Wu, J. Thomas Farrar, Bertrand Chapron, Stéphane Popinet, Luc Deike

AI总结:

本文利用直接数值模拟研究风驱增长-破碎波中的动量通量,发现破碎导致阻力突降,且平均阻力系数在高风速下饱和,该饱和由破碎动力学控制。

摘要:

我们通过直接数值模拟(DNS)求解气-水两相Navier-Stokes方程,研究了湍流空气边界层与增长-破碎波场之间的动量通量。充分发展的湍流气流驱动一个窄带波场增长,其振幅不断增加直至达到破碎条件。破碎事件导致波浪能量损失,并传递至水体,随后在风力驱动下重新增长。我们以增长-破碎循环为视角,重新审视了高风速条件下的动量通量分析,其特征由摩擦速度与波速之比 $u_\ast/c$ 在 $[0.3-0.9]$ 范围内表示。穿过界面的总动量通量以压力为主,在增长阶段随 $u_\ast/c$ 增大而增加,并在破碎期间急剧下降。破碎期间的阻力减小与气流分离、流动突然加速、平均流向速度剖面上移以及Reynolds剪切应力减小有关。我们通过将分析分为增长阶段和破碎阶段,并将它们视为独立的子过程,利用气动阻力系数来表征压力应力的减小和流动加速。在增长阶段阻力随 $u_\ast/c$ 增大而增加,而在破碎阶段阻力下降。对两个阶段取平均后,阻力系数在高 $u_\ast/c$ 下趋于饱和,这与实验室和现场条件下高风速时观测到的结果相当。我们的分析表明,这种饱和由破碎动力学控制。

英文摘要:

We investigate the momentum fluxes between a turbulent air boundary layer and a growing-breaking wave field by solving the air-water two-phase Navier-Stokes equations through direct numerical simulations (DNS). A fully-developed turbulent airflow drives the growth of a narrowbanded wave field, whose amplitude increases until reaching breaking conditions. The breaking events result in a loss of wave energy, transferred to the water column, followed by renewed growth under wind forcing. We revisit the momentum flux analysis in a high-wind speed regime, characterized by the ratio of the friction velocity to wave speed $u_\ast/c$ in the range $[0.3-0.9]$, through the lens of growing-breaking cycles. The total momentum flux across the interface is dominated by pressure, which increases with $u_\ast/c$ during growth and reduces sharply during breaking. Drag reduction during breaking is linked to airflow separation, a sudden acceleration of the flow, an upward shift of the mean streamwise velocity profile, and a reduction in Reynolds shear stress. We characterize the reduction of pressure stress and flow acceleration through an aerodynamic drag coefficient by splitting the analysis between growing and breaking stages, treating them as separate sub-processes. While drag increases with $u_\ast/c$ during growth, it drops during breaking. Averaging over both stages leads to a saturation of the drag coefficient at high $u_\ast/c$, comparable to what is observed at high wind speeds in laboratory and field conditions. Our analysis suggests this saturation is controlled by breaking dynamics.

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