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Near-Resonance of Diffraction Waves by an Array of Plates on Shallow Water in Oblique Waves

机译:斜波在浅水面上的一组平板对衍射波的近共振

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Near-resonance of diffraction waves by an array of plates rigidly fixed on shallow water is investigated under the assumption of linear long wave theory. The plates are assumed idetnical, equally spaced along the array, and infinitely long in breadth. Near-resonant modes occur between adjacent plates at critical wavenumbers in oblique waves. Considering the relationship between this near-resonant phenomenon and an eigenvalue problem of the wave diffraction, it is shown that near-resonant phenomena occur when transmitted wave takes its maximum and reflected wave vanishes. Relationships for the near-resonance between the wave incidence angle and the wavenumber are drawn as some curves. These curves of near-resonant points are confined in particular zones. We shall refer to these zones subsequently as the resonant zones. Each resonant zone has n-1 curves representing near-resonance, where n is the number of plates. The width of resonant zone itself is independent of the number of plates but depends on the spacing of plates, wavenumber, and incidence angle. The resonant zone becomes narrow as the wavenumber or incidence angle increases and the spacing of plates decreases. The curve representing near-resonance for the largest incidence angle gives critical angles of the near-resonance in this wave diffraction problem. The amplitudes of near-resonant modes on the curves situated in both edge sides of each resonant zone, become very large without limit as the number of plates increases.
机译:在线性长波理论的假设下,研究了由刚性固定在浅水中的一系列平板所产生的衍射波的近共振。假定这些板是理想的,沿阵列等距分布,并且宽度无限长。在斜波的临界波数下,相邻板之间会发生近共振模式。考虑到这种近共振现象与波衍射的特征值问题之间的关系,可以看出,当透射波达到最大值而反射波消失时,就会发生近共振现象。将波入射角和波数之间的近共振关系绘制为一些曲线。这些近共振点的曲线被限制在特定区域内。我们随后将这些区域称为谐振区域。每个共振区都有代表近共振的n-1条曲线,其中n是极板数。谐振区本身的宽度与板的数量无关,但取决于板的间距,波数和入射角。随着波数或入射角增加并且板的间距减小,谐振区域变窄。在该波衍射问题中,代表最大入射角的近共振的曲线给出了近共振的临界角。随着板数的增加,位于每个谐振区的两个边缘侧的曲线上的近谐振模的振幅变得非常大而没有限制。

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