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Numerical investigation of turbulence generation in non-breaking potential waves

机译:非破缺电位波中湍流产生的数值研究

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摘要

Theoretically, potential waves cannot generate the vortex motion, but scale considerations indicate that if the steepness of waves is not too small, Reynolds number can exceed critical values. This means that in presence of initial non-potential disturbances the orbital velocities can generate the vortex motion and turbulence. In the paper, this problem was investigated numerically on basis of full two-dimensional (x-z) equations of potential motion with the free surface in cylindrical conformal coordinates. It was assumed that all variables are a sum of the 2D potential orbital velocities and 3D non-potential disturbances. The non-potential motion is described directly with 3D Euler equations, with very high resolution. The interaction between potential orbital velocities and non-potential components is accounted through additional terms which include the components of vorticity. Long-term numerical integration of the system of equations was done for different wave steepness. Vorticity and turbulence usually occur in vicinity of wave crests (where the velocity gradients reach their maximum) and then spread over upwind slope and downward. Specific feature of the wave turbulence at low steepness (steepness was kept low in order to avoid wave breaking) is its strong intermittency: the turbulent patches are mostly isolated and intermittency grows with decrease of wave amplitude. Maximum values of energy of turbulence are in agreement with available experimental data. The results suggest that even non-breaking potential waves can generate turbulence, which thus enhances the turbulence created by the shear current.
机译:从理论上讲,势波不能产生涡旋运动,但是比例方面的考虑表明,如果波的陡度不太小,雷诺数可能会超过临界值。这意味着在存在初始非潜在扰动的情况下,轨道速度会产生涡旋运动和湍流。在本文中,在圆柱共形坐标系中具有自由表面的潜在运动的完整二维(x-z)方程的基础上,对该问题进行了数值研究。假定所有变量都是2D潜在轨道速度和3D非潜在干扰的总和。非势能运动使用3D Euler方程直接描述,具有很高的分辨率。潜在的轨道速度和非潜在的分量之间的相互作用是通过包括涡度分量在内的其他术语来说明的。对于不同的波陡度,对方程组进行了长期的数值积分。涡度和湍流通常发生在波峰附近(速度梯度达到最大),然后在上风向和向下传播。低陡波湍流的特定特征(为了避免波浪破碎,将陡度保持在较低的水平)是其强烈的间歇性:湍流斑块大多是孤立的,并且间歇性会随着波幅的减小而增大。湍流能量的最大值与可用的实验数据一致。结果表明,即使不破裂的势波也可以产生湍流,从而增强了由剪切电流产生的湍流。

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