Wave propagation in layered piezoelectric structures

1998 ◽  
Vol 83 (9) ◽  
pp. 4652-4659 ◽  
Author(s):  
A. A. Mesquida ◽  
J. A. Otero ◽  
R. R. Ramos ◽  
F. Comas
2021 ◽  
Vol 263 (2) ◽  
pp. 4303-4311
Author(s):  
Edson J.P. de Miranda ◽  
Edilson D. Nobrega ◽  
Leopoldo P.R. de Oliveira ◽  
José M.C. Dos Santos

The wave propagation attenuation in low frequencies by using piezoelectric elastic metamaterials has been developed in recent years. These piezoelectric structures exhibit abnormal properties, different from those found in nature, through the artificial design of the topology or exploring the shunt circuit parameters. In this study, the wave propagation in a 1-D elastic metamaterial rod with periodic arrays of shunted piezo-patches is investigated. This piezoelectric metamaterial rod is capable of filtering the propagation of longitudinal elastic waves over a specified range of frequency, called band gaps. The complex dispersion diagrams are obtained by the extended plane wave expansion (EPWE) and wave finite element (WFE) approaches. The comparison between these methods shows good agreement. The Bragg-type and locally resonant band gaps are opened up. The shunt circuits influence significantly the propagating and the evanescent modes. The results can be used for elastic wave attenuation using piezoelectric periodic structures.


2018 ◽  
Vol 142-143 ◽  
pp. 276-288 ◽  
Author(s):  
Dong-Jia Yan ◽  
A-Li Chen ◽  
Yue-Sheng Wang ◽  
Chuanzeng Zhang ◽  
Mikhail Golub

2006 ◽  
Vol 120 (4) ◽  
pp. 1964-1975 ◽  
Author(s):  
Mickaël Lematre ◽  
Guy Feuillard ◽  
Emmanuel Le Clézio ◽  
Marc Lethiecq

Electronics ◽  
2022 ◽  
Vol 11 (2) ◽  
pp. 176
Author(s):  
Gennady Kvashnin ◽  
Boris Sorokin ◽  
Nikita Asafiev ◽  
Viacheslav Prokhorov ◽  
Andrei Sotnikov

New theoretical and experimental results of microwave acoustic wave propagation in diamond-based multilayer piezoelectric structures (MPS) as “Me1/(Al,Sc)N/Me2/(100) diamond/Me3” and “Me1/AlN/Me2/(100) diamond/Me3” under three metal film depositions, including the change in the quality factor Q as a result of Me3 impact, were obtained. Further development of our earlier studies was motivated by the necessity of creating a sensor model based on the above fifth layered MPS and its in-depth study using the finite element method (FEM). Experimental results on the change in operational checkpoint frequencies and quality factors under the effect of film deposition are in satisfactory accordance with FEM data. The relatively small decrease in the quality factor of diamond-based high overtone bulk acoustic resonator (HBAR) under the metal layer effect observed in a wide microwave band could be qualified as an important result. Changes in operational resonant frequencies vs. film thickness were found to have sufficient distinctions. This fact can be quite explained in terms of the difference between acoustic impedances of diamond and deposited metal films.


Ultrasonics ◽  
2022 ◽  
Vol 118 ◽  
pp. 106559
Author(s):  
Kunpeng Chen ◽  
Zhi Wu ◽  
Yuan Jin ◽  
Jianying Hu ◽  
Jianke Du ◽  
...  

Nanomaterials ◽  
2021 ◽  
Vol 11 (9) ◽  
pp. 2270
Author(s):  
Olha Hrytsyna ◽  
Jan Sladek ◽  
Vladimir Sladek

The non-classical linear governing equations of strain gradient piezoelectricity with micro-inertia effect are used to investigate Love wave propagation in a layered piezoelectric structure. The influence of flexoelectricity and micro-inertia effect on the phase wave velocity in a thin homogeneous flexoelectric layer deposited on a piezoelectric substrate is investigated. The dispersion relation for Love waves is obtained. The phase velocity is numerically calculated and graphically illustrated for the electric open-circuit and short-circuit conditions and for distinct material properties of the layer and substrate. The influence of direct flexoelectricity, micro-inertia effect, as well as the layer thickness on Love wave propagation is studied individually. It is found that flexoelectricity increases the Love-wave phase velocity, while the micro-inertia effect reduces its value. These effects become more significant for Love waves with shorter wavelengths and small guiding layer thicknesses.


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