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NUMERICAL STUDY ON WAVE BOTTOM BOUNDARY LAYER OVER RIPPLES

机译:波纹波底边界层的数值研究

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Vortex ripple is widely formed in the coastal region. The vortex ripple enhance the separation of flow and turbulence, it plays a vital role in various coastal process, such as sediment transport, the wave attenuation and the mass transport due to wave. Nevertheless, the flow structure and sediment movement above vortex ripple has not been investigated owing to the complexity of the phenomena. Du Toit & Sleath (1981) used the Laser-Doppler to measure the flow over a ripple bed, the similar work was conducted by Sato S.J. et al. (1986), very detailed measurements of velocity closed to the bed over fixed smooth and rough bed are carried out using LAD. In resent years, most effort has been focused on obtaining a numerical solution of oscillatory flow over ripple, the first work was described by Lounguet-Higgins (1981), who used the discrete vortex model. Vittorri & Blondeaux (1991) treat a laminar flow situation by solving the vorticity transportation equations. Sato S.J. et al. (1986), Aydin (1987) and Tsujimoto et al (1991) used a two equation turbulent model k — ε to study the flow around the ripple and the suspended sediment concentration distribution. Recently, Fredsoe, J et al.(1999) have conducted experiments and numerical simulation by k — ω model to study the flow structure around the vortex ripples under wave action. In the present study, a numerical simulation system based on LES method is developed for analyzing flow structure and dynamic of vortex, the sub-grid-scale turbulent stress is evaluated by the Smagorinsky model (1963). The simplify marker and cell method (SMAC) is used to solve the basic equations in the the curvilinear coordinator system, and a detailed vortex dynamics is discussed.
机译:涡旋波纹在沿海地区广泛形成。涡旋波纹增强了流动和湍流的分离,它在各种海岸过程中起着至关重要的作用,例如泥沙输送,波浪衰减和波浪引起的质量输送。然而,由于现象的复杂性,尚未研究旋涡波纹上方的流动结构和沉积物运动。 Du Toit&Sleath(1981)用激光多普勒仪测量了波纹床上的流量,Sato S.J.等。 (1986年),使用LAD对固定的光滑和粗糙床上封闭床的速度进行了非常详细的测量。在最近的几年中,大部分精力都集中在获得波动上的振荡流的数值解上,第一项工作是由Lounguet-Higgins(1981)描述的,他使用了离散涡模型。 Vittorri&Blondeaux(1991)通过求解涡旋输运方程来处理层流情况。佐藤贤二等。 (1986年),Aydin(1987年)和Tsujimoto等人(1991年)使用两个方程式的湍流模型k-ε研究了围绕波纹的水流和悬浮的泥沙浓度分布。最近,Fredsoe,J等人(1999)通过k_ω模型进行了实验和数值模拟,研究了波浪作用下涡旋脉动周围的流动结构。在本研究中,开发了一种基于LES方法的数值模拟系统来分析涡流的流动结构和动力学,并利用Smagorinsky模型(1963年)评估了亚网格尺度的湍流应力。用简化标记和单元法(SMAC)求解曲线协调器系统中的基本方程,并讨论了详细的涡旋动力学。

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