Acta Physica Sinica, Volume. 68, Issue 12, 128101-1(2019)

Sound transmission in two-dimensional periodic poroelastic structures

Hou Qiao1, Zeng He1, Heng-Kun Zhang1, Wei-Cai Peng2, and Wen Jiang1、*
Author Affiliations
  • 1Department of Mechanics, Huazhong University of Science and Technology, Wuhan 430074, China
  • 2National Key Laboratory on Ship Vibration and Noise, China Ship Development and Design Center, Wuhan 430064, China
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    Figures & Tables(18)
    Schematic of the poroelastic composite structure and its substructures: (a) The poroelastic composite structure; (b) the equivalent model; (c) the OU boundary connection; (d) the OB boundary connection; (e) the forces in OU boundary case; (f) the forces in OB boundary case; (g) the forces in a simple spring-mass resonator.含多孔介质复合结构及其子结构示意图 (a) 含多孔介质复合结构; (b) 等效模型; (c) OU边界; (d) OB边界; (e) 板受力情况(OU边界); (f) 板受力情况(OB边界); (g) 弹簧振子受力
    Schematic of the composite-resonator-structure: (a) Composite resonator type A, two resonators placed in serial connection; (b) composite resonator type B, two resonators placed in composite connection.组合振子系统示意图 (a) 串联弹簧振子系统A; (b) 复合弹簧振子系统B
    Schematic of the arrangement of periodic resonators: (a) An array of simple resonators, denoted as multiple resonators (N1SR, with constant and ) or multiple kinds of resonators (NNSR, with different and ); (b) an array of composite resonators, denoted as multiple resonators (N1CR, with constant and ) or multiple kinds of resonators (NNCR, with different or ). The area in the dash-line denotes the periodic lattice, in panel (b), the composite resonator can be type B in Fig. 2周期振子排布方式示意图 (a) 简单振子周期分布, 按各个振子质量和特征频率分为多个振子情况 (N1SR, 和均保持恒定) 和多种振子情况 (NNSR, 或不相同); (b) 组合振子周期分布, 按振子部件质量和特征频率分为多个振子情况 (N1CR, 和均保持恒定) 和多种振子情况 (NNCR, 或不相同); 图中虚线框内部分为单个振子单元, (b)中虚线框部分可替换为 图2中B类组合振子
    Validation of the results here with previous results: (a) The diffuse case in Ref. [35]; (b) the oblique incident cases in Ref. [35]; (c) the composite poroelastic structure without resonator in Ref. [3]. The lines are results obtained here, while the marks are the results in the references.不同类型隔声结构验证算例 (a) 文献[35]随机入射情况; (b) 文献[35]斜入射情况; (c) 文献[3]含多孔介质复合结构; 其中, 各曲线为本文结果, 各标记为文献中结果
    Influence of porous material on the STL of the multiple-single-type-resonator composite structure with different characteristic frequencies: (a) OU case; (b) OB case. The solid lines correspond to cases with porous materials.有无多孔材料对含不同特征频率振子系统复合结构STL的影响 (a) OU边界情况; (b) OB边界情况; 有无多孔介质分别与相应实线和虚线对应
    The STL of multiple-single-type-resonator composite structure (fr = 300 Hz) with/without porous, and composite structure without resonators: (a) OU case; (b) OB case. Composite structure here with porous material: Porous + Resonator. Without porous material: Resonator. Composite structure without resonators: Porous.含相同简单振子系统复合结构(fr = 300 Hz)有无多孔介质及相应不含振子复合结构的STL (有多孔介质, Porous + Resonator; 无多孔介质, Resonator; 相应不含振子复合结构, Porous) (a) OU边界情况; (b) OB边界情况.
    Influences of resonators with different characteristic frequencies on the STL: (a) OU case; (b) OB case.采用不同特征频率简单振子系统对复合结构STL的影响 (a) OU边界; (b) OB边界
    (a) STL of OU and OB case in periodically-arranged single simple resonator case, and its displacement transmissibility Ti; (b) equivalent mass meq of a single resonator and the dynamic density of the equivalent plate.单一类型简单振子周期排布时 (a) OU, OB情况下STL及其位移传递率Ti; (b) 振子的等效质量meq和板等效动态密度
    Displacement transmissibility and dynamic mass of the mass components in the two composite resonators: (a1) Displacement transmissibility , of composite resonator type A; (a2) dynamic mass of composite resonator type A; (b1) displacement transmissibility , of composite resonator type B; (b2) dynamic mass of composite resonator type B.两类组合振子系统中质量块的位移传递率, 和动态质量(a1) 组合振子系统A中各质量块的位移传递率, ; (a2) 组合振子系统A的动态质量; (b1) 组合振子系统B中各质量块的位移传递率, ; (b2) 组合振子系统B的动态质量
    STL of the proposed composite structure with 4 identical simple resonators (Single resonator), composite resonators of type A or B versus its STL without any resonators (Without resonator) in a periodic lattice: (a) OU boundary case; (b) OB boundary case.复合结构周期间隔内分布4个相同简单振子(Single resonator), 组合振子A或组合振子B时的STL和不含振子复合结构(Without resonator)的STL (a) OU边界情况; (b) OB边界情况
    STL of the composite structure with NNSR configuration under two boundary cases: (a1), (a2) Case A; (b1), (b2) case B, . Here (a1) and (b1) correspond to OU case, (a2) and (b2) correspond to OB case.NNSR分布时OU, OB边界情况下的STL (a1), (a2) 情况A; (b1), (b2) 情况B, ; 其中, (a1)和(b1)为OU边界情况, (a2)和(b2)为OB边界情况
    STL of the proposed composite structure under NNCR configuration: (a1), (a2) Composite resonator type A; (b1), (b2) composite resonator type B. Here (a1) and (b1) correspond to OU case, (a2) and (b2) correspond to OB case.采用组合振子复合结构的STL (a1), (a2) 采用组合振子A; (b1), (b2) 采用组合振子B; 其中, (a1)和(b1)对应于OU边界情况, (a2)和(b2)对应于OB边界情况
    STL of different resonator system configuration: (a), (a1) OU case; (b), (b1) OB case. and correspond to simple resonator case NNSR. Type A and Type B correspond to composite resonator case NNCR.不同振子系统分布时STL对比 (a), (a1) OU边界情况; (b), (b1) OB边界情况; 和对应简单振子情况NNSR; Type A和Type B对应组合振子情况NNCR
    • Table 1. Abbreviations of the distribution of resonator systems and their meanings.

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      Table 1. Abbreviations of the distribution of resonator systems and their meanings.

      振子系统分布含义
      N1SR周期间隔内分布多个简单振子系统, 各振子系统 ${m_i}$${f_i}$均相等
      NNSR周期间隔内分布多种简单振子系统, 各振子系统 ${m_i}$${f_i}$不同
      N1CR周期间隔内分布多个组合振子系统, 各振子系统 $m_n^i$$f_n^i$均相等
      NNCR周期间隔内分布多种组合振子系统, 各振子系统 $m_n^i$$f_n^i$不同
    • Table 2. Parameters of plate and resonators.

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      Table 2. Parameters of plate and resonators.

      薄板空气域(20 ℃, 1 atm)简单振子
      h/mm E/GPa ν${\rho _{\rm{p}}}$/kg·m–3ρ/kg·m–3c0/m·s–1ha/mm fr/Hz γ
      1700.3327001.204343.2123000.2
    • Table 3. Parameters of the porous media used here

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      Table 3. Parameters of the porous media used here

      参数参数
      ${\rho _{\rm{s}}}$/kg·m–330$\epsilon$0.9
      ${\rho _{\rm{f}}}$/kg·m–31.204${\tau _\infty }$7.8
      ${E_{\rm{s}}}$/MPa 0.8(1+0.265 ${\rm{j}}$) ${\sigma _0}$/MKS rayls 25000
      ${\nu _s}$0.4hp/mm 50
    • Table 4.

      Parameters of the composite resonators.

      振子系统参数

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      Table 4.

      Parameters of the composite resonators.

      振子系统参数

      参数$\omega _1^i$$\omega _2^i$rs$\eta _1^i$$\eta _2^i$
      600 ${\text{π}}$10880.0750.06250.010.05
    • Table 5.

      Parameters of the composite resonators.

      组合振子系统参数

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      Table 5.

      Parameters of the composite resonators.

      组合振子系统参数

      参数rs$\eta _1^i$$\eta _2^i$
      0.0450.0400.010.05
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    Hou Qiao, Zeng He, Heng-Kun Zhang, Wei-Cai Peng, Wen Jiang. Sound transmission in two-dimensional periodic poroelastic structures[J]. Acta Physica Sinica, 2019, 68(12): 128101-1

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    Paper Information

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    Received: Jan. 28, 2019

    Accepted: --

    Published Online: Oct. 30, 2019

    The Author Email:

    DOI:10.7498/aps.68.20190164

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