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Bloch band gap of shallow-water waves over infinite arrays of parabolic bars and rectified cosinoidal bars and Bragg resonance over finite arrays of bars

机译:无限抛物线和整流余弦曲线上的浅水波的布洛赫带隙和有限阵列上的布拉格共振

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In this paper, eigenvalue problems of Bloch waves over an infinite array of equally spaced parabolic bars and rectified cosinoidal bars in shallow water are respectively studied. Both band expressions in closed form for the two eigenvalue problems are derived, which depend upon the dimensionless bar height with respect to water depth and the dimensionless bar width and spacing with respect to incident wavelength. It is found that the band-gap center associated with an infinite array of bars coincides well with the peak phase of Bragg resonance by any finite array of bars. For any fixed dimensionless bar height, a gap map as a bivariate function of the dimensionless bar width and spacing can be given. When both the dimensionless bar height and width are fixed, the band gap occurs periodically. When the dimensionless bar height is fixed, there exists a particular dimensionless bar width such that the band gap achieves its maximal width. Based on the gap maps, the well-known phenomenon of phase downshift can be visually and quantitatively explained, and the peak phase of Bragg resonant reflection by a finite array of bars can be well predicted, which is much more accurate than that predicted by Bragg's law.
机译:在本文中,分别研究了浅水中无限等距抛物线和整流余弦线阵列上的Bloch波特征值问题。推导了两个特征值问题的两个封闭形式的带表达式,这取决于相对于水深的无量纲条形高度和相对于入射波长的无量纲条形宽度以及间距。发现与无限条形阵列相关联的带隙中心与任何有限条形阵列的布拉格共振的峰值相位重合。对于任何固定的无量纲钢筋高度,可以给出作为无量纲钢筋宽度和间距的二元函数的间隙图。当无因次棒的高度和宽度都固定时,带隙会定期发生。当无因次棒高度固定时,存在特定的无因次棒宽度,以使带隙达到其最大宽度。基于间隙图,可以用视觉和定量方式解释众所周知的相移现象,并且可以很好地预测由有限条形组成的布拉格共振反射的峰值相位,这比由布拉格定律预测的准确得多。法。

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