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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >The phononic band gaps of Bragg scattering and locally resonant pentamode metamaterials
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The phononic band gaps of Bragg scattering and locally resonant pentamode metamaterials

机译:布拉格散射和局部共振五峰集石体隙差距

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In this paper, the phononic band structures of Bragg scattering and locally resonant pentamode metamaterials (PMs) with single and composite materials symmetric double-cone elements (SDCEs) are calculated by using the finite element method. The numerical results show that, for the Bragg scattering PMs with single material SDCEs, the phononic band gaps (PBGs) can be obtained while the top touch cone diameters (TTCDs) (i.e. d) are much smaller than the bottom touch cone diameters (i.e. D), and the variation range of the PBGs frequency is mainly determined by the TTCDs. This indicates that the Bragg scattering PMs with single material SDCEs can be investigated as a phonon crystal. On this basis, the locally resonant SDCE PMs can be designed by using the composite SDCEs instead of single material SDCEs, and the PBGs can be obtained under the 100 Hz. This finding provides a way to control the low-frequency acoustics waves by using small-sized SDCEs PMs. In addition, compared with the Bragg scattering PMs, the relative bandwidth of the first PBGs of the locally resonant PMs can be expanded at least 25 times. In the end, the effect of mass density rho and Young's modulus E of the composition material parameters of locally resonant SDCEs PMs on the PBGs is also studied by changing the parameters individually. The results show that the lower and upper edge and relative bandwidth of the first PBGs of locally resonant PMs with composite SDCEs are mainly impacted by the difference of the mass density rho between the two constituent materials, and the difference of the Young's modulus E between the two constituent materials has little effect on the PBGs.
机译:在本文中,通过使用有限元方法计算布拉格散射散射和局部共振五峰元材料(PMS)的局部谐振散射型二金属材料(PMS)。数值结果表明,对于具有单材料SDCE的布拉格散射PMS,可以获得声频带间隙(PBG),同时顶部触摸锥直径(TTCDS)(即D)远小于底部触摸锥直径(即D),并且PBGS频率的变化范围主要由TTCDS确定。这表明可以研究具有单材料SDCE的布拉格散射PM作为声子晶体。在此基础上,可以通过使用复合SDCE而不是单材料SDCE来设计局部谐振的SDCE PM,并且可以在100Hz下获得PBG。该发现提供了一种通过使用小型SDCES PM来控制低频声学波的方法。另外,与布拉格散射PMS相比,局部谐振PMS的第一PBG的相对带宽可以至少扩展为至少25次。最后,还通过单独改变参数来研究局部共振SDCES PMS的组合物材料参数的质量密度Rho和杨氏模量E的影响。结果表明,具有复合SDCE的局部谐振PMS的第一PBG的下边缘和上边缘和相对带宽主要受到两个组成材料之间质量密度ROO之间的差异的影响,以及杨氏模量e之间的差异两个组成材料对PBG影响不大。

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