Effect of initial stress on the propagation behavior of Love waves in a layered piezoelectric structure

Liu, H.; Wang, Z.K.; Wang, T.J.

doi:10.1016/s0020-7683(00)00009-3

Cited by 156 publications

(78 citation statements)

References 4 publications

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“…Therefore, it is much delightful to highlight the influence of these initial stress on the propagation of waves. Effect of initial stress on the propagation behaviour of Love waves in a layered piezoelectric structure was presented by Liu [12] et al Qian et al [13] have discussed propagation of Love waves in a piezoelectric layered structure with initial stresses. Biot [14] has delineated the influence of initial stress on elastic waves.…”

Section: Introductionmentioning

confidence: 99%

Torsional Wave Propagation in a Pre-Stressed Structure with Corrugated and Loosely Bonded Surfaces

Singh¹,

Sahu²

2017

Journal of Theoretical and Applied Mechanics

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An analytical model is presented to study the behaviour of propagation of torsional surface waves in initially stressed porous layer, sandwiched between an orthotropic half-space with initial stress and pre-stressed inhomogeneous anisotropic half-space. The boundary surfaces of the layer and halfspaces are taken as corrugated, as well as loosely bonded. The heterogeneity of the lower half-space is due to trigonometric variation in elastic parameters of the pre-stressed inhomogeneous anisotropic medium. Expression for dispersion relation has been obtained in closed form for the present analytical model to observe the effect of undulation parameter, flatness parameter and porosity on the propagation of torsional surface waves. The obtained dispersion relation is found to be in well agreement with classical Love wave equation for a particular case. The cases of ideally smooth interface and welded interface have also been analysed. Numerical example and graphical illustrations are made to demonstrate notable effect of initial stress, wave number, heterogeneity parameter and initial stress on the phase velocity of torsional surface waves.KEY WORDS: Corrugation, loose bonding, dispersion, orthotropic, heterogeneity LIST OF SYMBOLSK is the effective bonding parameter; k is the wave number; ς is the pure real number; g 1 (r) is the corrugated boundary surfaces of the porous layer; g 2 (r) is the corrugated boundary surfaces of lower the half-space;H is the thickness of the layer; z are the components of displacement for the upper half-space; D, F are the rigidity of upper half-space along radial and axial direction; P is the initial stress for the upper half-space; β 1 is the shear wave velocity for the upper half-space; J 1 (kr) is the Bessel's function of first order; ij are the components of stress for the porous layer; wz are the components of solid phase displacements for the porous layer; W r , W θ , W z are the components of fluid phase displacements for the porous layer; P 1 is the initial stress for the porous layer; u r , u θ , u z are the rotational components for the porous layer; α ij are the strain components for the porous layer; p f is the pressure in the fluid of porous layer; π is the porosity of the poroelastic layer; ρ rr , ρ rθ , ρ θθ are the mass coefficients;is the density the solid-liquid for the porous layer; p s , p f are the mass densities of the solid and liquid for the porous layer;N , L are the rigidities of the porous layer, along radial and axial direction;Q is the porosity parameter for the porous layer; β 2 is the shear wave velocity of porous layer; τ ij are stress components for the lower inhomogeneous anisotropic half-space; α is the heterogeneity parameter for the lower half-space; P is the initial stress for the lower half-space; ρ 3 is the density of the lower medium; β 3 is the shear wave velocity for the lower half-space; L , A are the rigidity of the lower half-space along radial and axial direction;Ω 1 is bonding parameter of common interface of upper half-space and ...

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Section: Introductionmentioning

confidence: 99%

Torsional Wave Propagation in a Pre-Stressed Structure with Corrugated and Loosely Bonded Surfaces

Singh¹,

Sahu²

2017

Journal of Theoretical and Applied Mechanics

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“…Therefore, there is a great deal of research literatures on piezoelectric functional devices with dielectric coating. [26][27][28] Nowacki et al 29,30 obtained exact solutions for a piezoelectric coating-substrate structure in the form of Fourier integrals and discussed the convergence. A method of a spherical acoustic transducer that consists of a piezoelectric sphere substrate and an elastic coating is presented by Georgea and Ebenezer.…”

Section: Introductionmentioning

confidence: 99%

Study on the interactions between the coatings of electric conductor or dielectric media and piezoelectric substrate in the piezoelectric functional devices

2017

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Because that most of piezoelectric functional devices are combined with the coatings of electric conductor or dielectric media and the piezoelectric substrate, the study on the interactions between them is valuable for their advanced design. In this paper, a method for the electro-mechanical coupling fields in these piezoelectric functional devices is presented. Firstly, the two-dimensional Green’s function for a normal line force or line charge is derived. Then, based on the obtained Green’s function, the interaction mechanism between the coatings of electric conductor or dielectric media and the piezoelectric substrate is studied. Finally, the electro-mechanical coupling fields under arbitrary loads are obtained by superposition principle and Gauss integration. Numerical results show that this method has high computational precision, efficiency and stability. And it can be used to improve the reliability and working performance of the piezoelectric functional device effectively.

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“…Son et al [10] and Du et al [11] discuss the effect of initial stress on propagation of an SH wave in piezoelectric layers. Liu et al [12] and Qian et al [13] study the Love wave propagation in a piezoelectric structure in the presence of initial stress and found that the phase velocity depends on the value of stress at the A. M. Gaur (B) · D. S. Rana Department of Instrumentation (I.I.E), Kurukshetra University, Kurukshetra, Haryana, 136119 India E-mail: gauranshu10@gmail.com interface. A three-layer model was presented by Li et al [14] and investigated the effect of an intermediate soft layer on the propagation characteristics of Love waves.…”

Section: Introductionmentioning

confidence: 99%

Dispersion relations for SH waves propagation in a porous piezoelectric (PZT–PVDF) composite structure

Gaur

Rana

2015

Acta Mech

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The propagation of shear horizontal waves in a porous piezoelectric composite structure is investigated analytically in this paper. A two-layer structure comprised of perfectly bonded piezoelectric layers is considered. The solution of mechanical displacement and electrical potential is found by solving the constitutive equation for a porous piezoelectric composite structure. Then the dispersion relation is derived for the wave propagation along the direction normal to layering and in the direction of layering. The results obtained from the investigation show the dependence of the wave number on the thickness of the alternative layer in piezoelectric material. Also the phase velocity has been significantly influenced by the variation of elastic constant and porosity. The results provide a theoretical framework for designing and development of underwater acoustic devices for sensing and nondestructive testing.

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Effect of initial stress on the propagation behavior of Love waves in a layered piezoelectric structure

Cited by 156 publications

References 4 publications

Torsional Wave Propagation in a Pre-Stressed Structure with Corrugated and Loosely Bonded Surfaces

Torsional Wave Propagation in a Pre-Stressed Structure with Corrugated and Loosely Bonded Surfaces

Study on the interactions between the coatings of electric conductor or dielectric media and piezoelectric substrate in the piezoelectric functional devices

Dispersion relations for SH waves propagation in a porous piezoelectric (PZT–PVDF) composite structure

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