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A Coupled-Mode Technique for Wave-Current Interactionin Variable Bathymetry Regions

机译:可变测深区域中波流相互作用的耦合模式技术

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A coupled-mode technique for wave-current interaction is presented,rnwith application to the problem of wave scattering by steady currents inrnvariable bathymetry regions, and current variations on various scales.rnWe consider obliquely incident waves on a horizontally nonhomogeneousrncurrent in a variable-depth strip, which is characterizedrnby straight and parallel bottom contours. The flow associated with therncurrent is assumed to be parallel to the bottom contours (along-axisrncurrent) and it is considered to be known. In a finite subregionrncontaining the bottom irregularity we assume an arbitrary horizontalrncurrent structure. Outside this region, the current is assumed to bernuniform (or zero). At a first-order of approximation the wave flow isrnassumed to be irrotational, I.e. the vorticity of the total field is the samernwith the vorticity associated with the current. Then, restrictingrnourselves to linear, monochromatic (harmonic) waves of absoluternfrequency ω, the wave potential, including the scattering effect by therncurrent, is obtained as a solution to the modified Helmholtz equation,rnsubject to the free-surface boundary condition formulated with respectrnto the intrinsic frequency, the bottom boundary condition, and thernconditions at infinity. Based on an appropriate variational principle, inrnconjunction with a rapidly-convergent local-mode series expansion ofrnthe wave field in a finite subregion containing the current variation andrnthe bottom irregularity, a coupled-mode system is obtained that can bernconsidered as a generalization of the one derived by Athanassoulis &rnBelibassakis (1999). The present approach can be considered as anrnextension of the works by Smith (1983, 1987), and some of its mainrnfeatures are that it can be further elaborated to treat lateralrndiscontinuities (e.g. vertical vortex sheets) and more general verticalrncurrent profiles with cross-jet component, and to include the effects ofrnweak nonlinearity.
机译:提出了一种波流相互作用的耦合模式技术,并将其应用于由恒定电流不变的测深区域引起的波散射问题以及各种规模的电流变化。rn我们考虑了在可变深度带中水平非均匀电流上的斜入射波,其特征是笔直和平行的底部轮廓。假定与电流相关的流动与底部轮廓(沿轴电流)平行,并且被认为是已知的。在包含底部不规则性的有限子区域中,我们采用任意水平电流结构。在该区域之外,假定电流是均匀的(或零)。在近似一阶时,波流被假定为不旋转的,即总场的涡度与电流相关的涡度相同。然后,将我们自己限制在绝对频率为ω的线性,单色(谐波)波上,得到波势,包括由电流引起的散射效应,作为修正的亥姆霍兹方程的解,并以关于本征的自由表面边界条件为条件频率,底部边界条件和无穷大条件。基于适当的变分原理,在包含电流变化和底部不规则性的有限子区域中,波场在快速收敛的局部模式级数展开下的不相交,获得了可以被认为是对导出模态的推广的耦合模式系统。由Athanassoulis&rnBelibassakis(1999)。目前的方法可以认为是Smith(1983,1987)的工作的扩展,其一些主要特征是可以进一步完善以处理横向不连续性(例如垂直涡旋片)和带有交叉射流分量的更一般的垂直电流剖面,并包括弱非线性的影响。

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