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Abstract propagation of plane waves in thermo-piezoelectric media with thermal relaxation times in the framework of generalized theories of thermoelasticity has been become a topic for a lot of investigations in recent years. These investigations are considered to be important because of their possible extensive applications in various branches of science and technology. They also have a lot of applications in many natural scientific fields such as: astrophysics, geophysics, seismology, acoustics, radio electronics, communications and computer technology. The principal aim of this thesis is to investigate and find solutions of some problems associated with wave propagation in thermo-piezoelectric media under the effect of thermal relaxation times. This thesis consists of five chapters, some appendixes, Arabic abstract, English summary and a list of references. The contents of the chapters may be reviewed as follows: Chapter one: In this chapter, we present a general introduction on the subject of this thesis, and we recall some of the useful definitions and many of basic concepts. Next, the importance of the piezoelectric, thermoelastic and thermo-piezoelectric materials is introduced. Finally, the basic equations and constitutive relations for an anisotropic thermo-piezoelectric materials with the existence the thermal relaxation times are given. Chapter two: The objective of this chapter is to study the bulk acoustic wave (BAW) propagation velocities in transversely isotropic piezoelectric materials, Aluminum Nitride, Zinc Oxide, Cadmium sulfide and Cadmium Selenide. 5 The BAW velocities are computed for each direction by solving the Christoffel’s equation based on the theory of acoustic waves in anisotropic solids exhibiting piezoelectricity. These values are calculated numerically and implemented on a computer by Bisection Method Iterations Technique (BMIT). The modifications of the BAW velocities caused by the piezoelectric effect are graphically compared with the velocities in the corresponding non-piezoelectric materials. The results obtained in this study can be applied to signal processing, sound systems and wireless communication in addition to the improvement of surface acoustic wave (SAW) devices and military defense equipment. Chapter three: In this chapter, the well-established two-dimensional mathematical model for linear pyroelectric materials is employed to investigate the reflection of waves at the boundary between a vacuum and an elastic, transversely isotropic, pyroelectric material. A comparative study between the solutions of (a) classical thermoelasticity, (b) Lord-Shulman theory and (c) Green-Lindsay theory equations, characterized by none, one and two relaxation times respectively, is presented. Suitable boundary conditions are considered in order to determine the reflection coefficients when incident elasto-electro-thermal waves impinge the free interface. It is established that, in the quasi-electrostatic approximation, three different classes of waves: (i) two principally elastic waves, namely, a quasilongitudinal Primary (qP) wave and a quasi-transverse Secondary (qS) wave; and (ii) a mainly thermal (qT) wave. The observed electrical effects are, on the other hand, a direct consequence of mechanical and thermal phenomena due to pyroelectric coupling. The computed reflection coefficients of plane qP waves are found to depend upon the angle of incidence, the elastic, electric and thermal parameters of the medium, as 6 well as the thermal relaxation times. Finally, the reflection coefficients are computed for Cadmium selenide (CdSe) observing the influence of (i) the anisotropy of the material, (ii) the electrical potential and (iii) temperature variations and (iv) the thermal relaxation times on the reflection coefficients. Chapter four: In this chapter, the basic equations of motion, of Gauss and of heat conduction, together with constitutive relations for pyro- and piezoelectric media, are presented. Three thermoelastic theories are considered: classical dynamical coupled theory, the Lord–Shulman theory with one relaxation time and Green and Lindsay theory with two relaxation times. For incident elastic longitudinal, potential electric and thermal waves, referred to as q P, φ-mode and T-mode waves, which impinge upon the interface between two different transversal isotropic media, reflection and refraction coefficients are obtained by solving a set of linear algebraic equations. A case study is investigated: a system formed by two semiinfinite, hexagonal symmetric, pyroelectric–piezoelectric media, namely Cadmium Selenide (CdSe) and Barium Titanate (BaTiO3). Numerical results for the reflection and refraction coefficients are obtained, and their behavior versus the incidence angle is analyzed. The interaction with the interface give rises to different kinds of reflected and refracted waves: (i) two reflected elastic waves in the first medium, one longitudinal (qPwave) and the other transversal (qSV-wave), and a similar situation for the refracted waves in the second medium; (ii) two reflected potential electric waves and a similar situation for the refracted waves; (iii) two reflected thermal waves and a similar situation for the refracted waves. The amplitudes of the reflected and refracted waves are functions of the incident angle, of the thermal relaxation times and of the media elastic, 7 electric, thermal constants. This study is relevant to signal processing, sound systems, wireless communications, surface acoustic wave devices and military defense equipment. Chapter Five: In this chapter, a mathematical model of the effect of the rotation on horizontally shear wave (SH-wave) propagation in a piezoelectric halfspace covered by a semiconductor film is investigated analytically. The semiconducting layer is rotating with a uniform angular velocity. The interface between the piezoelectric substrate and the semiconductor layer is imperfectly bonded. The surfaces of the bilayer system are free of traction, electrically shorted or open are considered. The governing equations of the mechanical displacement and electrical potential function under the effect of rotation are obtained by solving the coupled electromechanical field equations of the piezoelectric half-space and the semiconductor film. The exact frequency equations of SH waves are derived. The numerical examples are given to illustrate the effects of rotation and electromagnetic boundary conditions, the different values of the film thickness and wave number on the dispersion behaviors. Finally, the effect of the rotation on the frequency equation is investigated in detail for piezoelectric ceramics PZT-5H and semiconductor silicon. The obtained results provide a predictable and theoretical basis for applications of piezoelectric and semiconductor composites to acoustic wave devices. |