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Generation Mechanisms and Sources of Vorticity Within a Spilling Breaking Wave

机译:在溢出波中的产生机制和涡旋源

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Sources of vorticity are examined for a spilling breaking wave. Through the use of a honeycomb/screen section, spilling breaking waves are generated and examined. Two cases were studied. For the first case, based on the breaker height, the Reynolds and Froude numbers were 7370 and 2.04, respectively. The breaker is preceded by 1 mm wavelength capillary waves, with the largest amplitude to wavelength ratio equal to 0.18. For this case, it is found that the dominant source of vorticity flux is a viscous process, and is due to the deceleration of a thin layer of the surface fluid. Furthermore, a thin free surface fluid layer is found to precede wave breaking that moves at a faster speed with respect to the fluid directly beneath it and to the fluid bulk. For the second case, also based on the wave height, the Reynolds and Froude numbers were 1500 and 1.35, respectively. No breaking is observed for this case; rather a capillary-gravity wave is observed with 4 mm wavelength capillaries preceding the gravity wave. The largest amplitude to wavelength ratio of these capillary is 0.28. This case shows that capillary waves do not contribute to the vorticity flux, rather the only dominant source of the vorticity flux into the flow is the free surface fluid deceleration. Lastly, similar to case 1, a thin free-surface fluid layer, which moves faster than the fluid beneath it and to the fluid bulk is found preceding the capillary-gravity wave.
机译:检查涡旋源,用于溢出波浪。通过使用蜂窝/屏幕部分,产生并检查溢出破碎波。研究了两种情况。对于第一种情况,基于断路器高度,雷诺和弗劳德数分别为7370和2.04。断路器在波长毛细波之前的比例为1mm,波长比的最大幅度等于0.18。对于这种情况,发现主导涡流源极是粘性过程,并且是由于表面流体薄层的减速。此外,发现薄的自由表面流体层以先成的波断裂,其以更快的速度相对于流体直接在其下方和流体堆积中移动。对于第二种情况,还基于波浪高度,雷诺和弗劳德数分别为1500和1.35。这种情况没有观察到任何破坏;相反,在重力波之前观察到毛细管 - 重力波。这些毛细管的最大幅度与这些毛细管的波长比为0.28。这种情况表明,毛细波对Vorticity通量没有贡献,而是涡流通量的唯一主导源流入流量是自由表面流体减速度。最后,类似于壳体1的薄型自由表面流体层,其比毛细管 - 重力波在其下方的流体和流体块状的流体移动。

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