共查询到16条相似文献,搜索用时 78 毫秒
1.
借助于平面波展开法分析了二维复式格子声子晶体能带结构,计算了铝合金柱体按周期性结构排列在空气中形成的二维固/气复合体系的声子晶体,给出了复式蜂窝格子和复式Kagome格子的能带结构,进而对比分析了复式格子和简单格子的能带结构特性.结果表明,与简单格子相比,复式格子的带隙出现在频率相对较低的位置;在f=0.091—0.6046范围内,将声子晶体排列为复式格子要优于简单格子,可以得到更宽带隙.此外,引入了带隙分布图,讨论了填充系数f对带隙数目、带隙宽度以及带隙上下边界频率的影响.
关键词:
声子晶体
复式格子
带隙
平面波算法 相似文献
2.
3.
介绍了平面波算法计算声子晶体带结构的分析过程,计算了二维双组分液相体系声子晶体的带结构.结果表明,四氯化碳/水银体系比水银/四氯化碳体系更容易产生带隙.随分散相填充分数f的增加,四氯化碳/水银体系声子晶体带隙宽度ΔΩ先增加,后减小,当f=0229时,有最大值ΔΩ=0549;水银/四氯化碳体系的带隙宽度一直增大,当f=0554时,有最大值ΔΩ=0515;f一定时,改变分散相单元的几何尺寸和点阵常数,带隙宽度ΔΩ保持不变.
关键词:
声子晶体
声子带隙
平面波算法
带结构 相似文献
4.
5.
通过引入振动力学中的连续系统离散化的思想,将一维集中质量法延伸至二维,提出一种二维声子晶体带隙特性计算的集中质量法. 进而采用该算法对两种正方晶格的二维声子晶体的带结构进行了计算,计算结果与传统的平面波展开法相符合. 通过对计算结果以及两种算法收敛性的分析,发现集中质量法的收敛性对组成声子晶体的不同材料弹性参数差不敏感,这使得该算法在计算大弹性常数差二维声子晶体的带隙特性时较平面波展开法收敛速度更快. 此外,集中质量法对二维声子晶体单元形状没有特殊要求,这使得它更加适用于声子晶体带隙特性的计算.
关键词:
声子晶体
声子带隙
集中质量法 相似文献
6.
7.
8.
9.
三维声子晶体带结构研究 总被引:1,自引:0,他引:1
运用平面波展开法计算由长方体散射物以面心立方结构排列于基体中形成的三维声子晶体的带结构,研究不同组分材料、散射物的填充率和长方体散射物的高与长之比 R_(HL)对带隙的影响.结果表明,将质量密度和波速大的散射体放在质量密度和波速小的基体中所形成的三维(面心立方)固态声子晶体有利于带隙的产生;散射体的填充率为中间值时带隙最宽;散射体的对称性强烈影响带隙,当 R_(HL)大于等于1时,带隙宽度随 R_(HL)的增加而减小,相反,当 R_(HL)小于1时,带隙宽度随 R_(HL)的增加而增加. 相似文献
10.
11.
We present a detailed theoretical study on the acoustic band structure of two-dimensional(2D)phononic crystal.The 2D phononic crystal with parallelogram lattice structure is considered to be formed by rigid solid rods embedded in air.For the circular rods,some of the extrema of the acoustic bands appear in the usual high-symmetry points and,in contrast,we find that some of them are located in other specific lines.For the case of elliptic rods,our results indicate that it is necessary to study the whole first Brillouin zone to obtain rightly the band structure and corresponding band gaps.Furthermore,we evaluate the first and second band gaps using the plane wave expansion method and find that these gaps can be tuned by adjusting the side lengths ratio R,inclined angleθand filling fraction F of the parallelogram lattice with circular rods.The results show that the largest value of the first band gap appears atθ=90°and F=0.7854.In contrast,the largest value of the second band gap is atθ=60°and F=0.9068.Our results indicate that the improvement of matching degree between scatterers and lattice pattern,rather than the reduction of structural symmetry,is mainly responsible for the enhancement of the band gaps in the 2D phononic crystal. 相似文献
12.
Much of previous work has been devoted in studying complete band gaps for bulk phononic crystal (PC). In this paper, we theoretically investigate the existence and widths of these gaps for PC plates. We focus our attention on steel rods of square cross sectional area embedded in epoxy matrix. The equations for calculating the dispersion relation for square rods in a square or a triangular lattice have been derived. Our analysis is based on super cell plane wave expansion (SC-PWE) method. The influence of inclusions filling factor and plate thickness on the existence and width of the phononic band gaps has been discussed. Our calculations show that there is a certain filling factor (f = 0.55) below which arrangement of square rods in a triangular lattice is superior to the arrangement in a square lattice. A comparison between square and circular cross sectional rods reveals that the former has superior normalized gap width than the latter in case of a square lattice. This situation is switched in case of a triangular lattice. Moreover, a maximum normalized gap width of 0.7 can be achieved for PC plate of square rods embedded in a square lattice and having height 90% of the lattice constant. 相似文献
13.
提出了一种新型的非对称性散射体的二维六角晶格光子晶体结构–-太极形介质柱光子晶体. 利用平面波展开法从理论研究这种光子晶体结构的能带特性以及结构参数对完全禁带的影响. 研究表明:散射体对称性的打破, TE模和TM模能带宽度和数目都会有所增加, 有益于获得更宽的完全禁带以及更多条完全禁带.通过参数优化, 发现在ε = 17, R=0.38 μm, r=0.36R, θ = 0° 时, 获得最大完全带隙宽度0.0541(ωa/2πc); 在ε = 16, R=0.44, r=0.2R, θ = 0°时, 光子晶体完全带隙数目最多达到8条.
关键词:
光子晶体
禁带
平面波展开 相似文献
14.
A wavelet-based method was developed to compute elastic band gaps of one-dimensional phononic crystals. The wave field was
expanded in the wavelet basis and an equivalent eigenvalue problem was derived in a matrix form involving the adaptive computation
of integrals of the wavelets. The method was then applied to a binary system. For comparison, the elastic band gaps of the
same one-dimensional phononic crystals computed with the wavelet method and the well-known plane wave expansion (PWE) method
are both presented in this paper. The numerical results of the two methods are in good agreement while the computation costs
of the wavelet method are much lower than that of PWE method. In addition, the adaptability of wavelets makes the method possible
for efficient band gap computation of more complex phononic structures.
Supported by the National Natural Science Foundation of China (Grant No. 10632020) 相似文献
15.
16.
Acoustic bands are studied numerically for a Lamb wave propagating in an anti-symmetric structure of a one-dimensional periodic plate by using the method of supercell plane-wave expansion. The results show that all the bands are pinned in pairs at the Brillouin zone boundary as long as the anti-symmetry remains and acoustic band gaps (ABGs) only appear between certain bands. In order to reveal the relationship between the band pinning and the anti-symmetry, the method of eigenmode analysis is introduced to calculate the displacement fields of different plate structures. Further, the method of harmony response analysis is employed to calculate the reference spectra to verify the accuracy of numerical calculations of acoustic band map, and both the locations and widths of ABGs in the acoustic band map are in good agreement with those of the reference spectra. The investigations show that the pinning effect is very sensitive to the anti-symmetry of periodic plates, and by introducing different types of breakages, more ABGs or narrow pass bands will appear, which is meaningful in band gap engineering. 相似文献