Evanescent waves in hybrid poroelastic metamaterials with interface effects

被引:4
|
作者
Zhang, Shu-Yan [1 ]
Luo, Jia-Chen [2 ]
Wang, Yan-Feng [3 ]
Laude, Vincent [4 ]
Wang, Yue-Sheng [1 ,3 ]
机构
[1] Beijing Jiaotong Univ, Inst Engn Mech, Beijing 100044, Peoples R China
[2] Dalian Univ Technol, Dept Engn Mech, State Key Lab Struct Anal Ind Equipment, Dalian 116023, Peoples R China
[3] Tianjin Univ, Sch Mech Engn, Dept Mech, Tianjin 300350, Peoples R China
[4] Univ Bourgogne Franche Comte, Inst FEMTO ST, CNRS, F-25030 Besancon, France
基金
中国国家自然科学基金;
关键词
Hybrid poroelastic metamaterials; Interface effects; Single-phased and poroelastic system; Complex band structures; ACOUSTIC BAND-GAPS; ELASTIC-WAVES; PLANE-WAVES; BOUNDARY-CONDITIONS; PHOTONIC CRYSTALS; PHONONIC CRYSTAL; SEISMIC-WAVES; REFLECTION; TRANSMISSION; PROPAGATION;
D O I
10.1016/j.ijmecsci.2023.108154
中图分类号
TH [机械、仪表工业];
学科分类号
0802 ;
摘要
The propagation of evanescent waves in hybrid poroelastic metamaterials is investigated by considering interface effects. Hybrid metamaterials consist of a single-phased (acoustic or elastic) medium and a poroelastic medium. To establish the finite element model of elastic/poroelastic and fluid/poroelastic interfaces, weak inte-gral forms of wave equations for elastic, fluid, and poroelastic media and boundary conditions at the interfaces between different media are first given. Next, the expressions for displacement and pressure in the frame of Bloch's theorem are substituted into the dynamical equations to obtain general forms suitable for periodic metamaterials, from which the complex band structure and the frequency response of hybrid metamaterials are calculated. The influence of geometrical and material parameters, as well as the viscosity of the pore fluid on the propagation of elastic waves are discussed. The results and discussions show that flat bands and narrow locally resonant band gaps appear for elastic/poroelastic metamaterials. A quasi-resonance Bragg band gap is formed in the case of an elastic inclusion in a poroelastic matrix. Furthermore, a transition from an avoided crossing to a wave-number band gap is obtained by adjusting the geometrical and material parameters of the elastic inclusion. For the case of fluid inclusion in a poroelastic matrix with the open-pore interface, a cut-off frequency for the fast longitudinal wave is observed. However, only an avoided crossing is produced for the sealed-pore interface. For both cases, the phase velocity of the shear vertical (SV) wave decreases faster than that of the slow longitudinal wave as the radius of the inclusion increases. When the viscosity of the pore fluid is considered for elastic inclusion in a poroelastic matrix, the transmission dip at the 'quasi-resonance Bragg' band gap disappears. However, the transmission dip in the locally resonant band gap of the SV wave becomes slightly shallower and smoother than in the inviscid case. This study is relevant to practical applications of hybrid single-phased and poroelastic metamaterials, e.g., for coastal engineering and civil engineering.
引用
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页数:22
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