Impacts of wave age on turbulent flow and drag of steep waves

Peter P. Sullivan , Michael L. Banner , Russel P. Morison , William L. Peirson
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引用次数: 9

Abstract

Turbulent flow over steep steady and unsteady wave trains with varying height h(x, t) and propagation speed c is simulated using large-eddy simulation (LES) in a wind-wave channel [17]. The imposed waveshape with steady wave trains is based on measurements of incipient and active breaking waves collected in a wind-wave tank, while a numerical wave code is used to generate an unsteady evolving wave train (or group) [3]. For the adopted waveshapes, process studies are carried out varying the wave age c/u* from ~ 1 to 10: the airflow friction velocity is u*. Under strong wind forcing or low wave age c/u* ~ 1, highly intermittent airflow separation is found in all simulations and the results suggest separation near a wave crest occurs prior to the onset of wave breaking. As wave age increases flow separation is delayed or erased for both steady and unsteady wave trains. Flow visualization shows that near the wave surface vertical velocity w and waveslope ∂h/∂x are positively correlated at c/u* ~ 1 but are negatively correlated at c/u* = 10. The vertical speed of the underlying wave oscillations depends on the local waveslope, increases with phase speed, and is a maximum on the leeward side of the wave. Vigorous boundary movement [8] appears to alter the unsteady flow separation patterns which leads to a reduction in form (pressure) drag as wave age increases. For example, the pressure contribution to the total drag of the active breaker wave train decreases from 74% at c/u* = 1.23 to less than 20% at c/u* = 10. Critical layer dynamics appears to play a secondary role in the air-wave coupling over steep waves, but requires further investigation. For all simulations, the form drag is found to be strongly dependent on both waveslope ∂h/∂x and wave age c/w*. The simulations are in good agreement with experimental results for turbulent flow over steep waves under strong wind forcing.

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波龄对陡波湍流和阻力的影响
采用大涡模拟(large-eddy simulation, LES)在风浪通道中模拟了不同高度h(x, t)和传播速度c的陡峭定常和非定常波列上的湍流[17]。施加的稳定波列波形是基于风浪槽中收集的初始破碎波和活动破碎波的测量,而数值波码则产生非定常演化波列(或组)[3]。对于所采用的波形,将波龄c/u*从~ 1变化到10,进行了过程研究,气流摩擦速度为u*。在强风强迫或低波龄c/u* ~ 1条件下,所有模拟均存在高度间歇的气流分离,结果表明在破波开始之前,在波峰附近发生气流分离。随着波龄的增加,不论是定常波列还是非定常波列,流动分离都被延迟或消除。流场可视化显示,近波面垂直速度w与斜率∂h/∂x在c/u* = 1处呈正相关,在c/u* = 10处呈负相关。下伏波振荡的垂直速度取决于局部波形,随着相速的增加而增加,并且在波的背风侧达到最大值。剧烈的边界运动[8]似乎改变了非定常流分离模式,导致形式(压力)阻力随着波龄的增加而减少。例如,在c/u* = 1.23时,压力对主动断路器波列总阻力的贡献从74%下降到c/u* = 10时的20%以下。临界层动力学似乎在陡波上空的空气波耦合中起次要作用,但需要进一步研究。对于所有的模拟,形式阻力被发现强烈依赖于波形∂h/∂x和波龄c/w*。模拟结果与实验结果吻合较好。
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