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首页> 外文期刊>Acta Physica Polonica. A >Phononic Band Gap Width Control through Structural and Material Parameters in Two-Dimensional Phononic Crystals
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Phononic Band Gap Width Control through Structural and Material Parameters in Two-Dimensional Phononic Crystals

机译:通过结构和材料参数控制二维声子晶体中的声子带隙宽度

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摘要

The phononic band structures of two-dimensional solid phononic crystals with different lattice and scatterer symmetry are studied numerically, with three types of lattice (square, triangular, and rectangular) and four different scatterer shapes (circle, hexagon, square, and rectangle) considered. XY and Z vibration modes are investigated separately. Two types of phononic crystal are considered: one composed of high-density rods embedded in a low-density matrix, the other of low-density rods in a high-density matrix. In the former case, lattice type and polarization being fixed, the broadest gaps are obtained when the symmetry of the rods corresponds to that of the lattice (the shape of a rod is identical with that of the first Bril-louin zone); the largest gap width values are observed in triangular lattice--based crystals (compared to those based on the square and rectangular lattices), the shape of the corresponding first Brillouin zone being closest to a circle. These rules do not apply to structures in which the density of the rod material is lower than that of the matrix. In this case, when the symmetry of the rods corresponds to that of the lattice, gaps either fail to appear at all, or are much narrower than in other configurations. The effect of other material parameter values (such as the longitudinal and transversal velocity values) on the relation between the energy gap width and the scatterer symmetry is found to be much lesser.
机译:数值研究了具有不同晶格和散射对称性的二维固体声子晶体的声带结构,考虑了三种类型的晶格(正方形,三角形和矩形)和四种不同的散射体形状(圆形,六边形,正方形和矩形) 。分别研究XY和Z振动模式。考虑两种类型的声子晶体:一种由嵌入低密度矩阵中的高密度棒组成,另一种由高密度矩阵中的低密度棒组成。在前一种情况下,晶格类型和极化是固定的,当杆的对称性与晶格的对称性相对应时(杆的形状与第一Bril-Loin区的形状相同),可以得到最宽的间隙。在基于三角形晶格的晶体中观察到最大的间隙宽度值(与基于方形和矩形晶格的晶体相比),相应的第一布里渊区的形状最接近圆形。这些规则不适用于棒材料的密度低于基体材料的密度的结构。在这种情况下,当杆的对称性对应于晶格的对称性时,间隙根本不出现,或者比其他构造窄得多。发现其他材料参数值(例如纵向和横向速度值)对能隙宽度和散射体对称性之间关系的影响要小得多。

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