Nowacki Static and Dynamic Coupled Fields in Bodies with Piezoeffects or Polarization Gradient

2006
ISBN: 978-3-540-31670-1
Verlag: Springer
Format: PDF
Kopierschutz: 1 - PDF Watermark

E-Book, Englisch, Band 26, 209 Seiten, eBook

Reihe: Lecture Notes in Applied and Computational Mechanics

This book is devoted to the theory of coupled electro-magneto-thermo-elastic fields excited in different bodies by various sources, both static and dynamic. It presents the classical piezoelectric and piezomagnetic effects, the Mindlin’s electroelastic coupling due to a polarization gradient, and different combinations of these effects with thermoelasticity.

Zielgruppe

Research

Autoren/Hrsg.

Nowacki, Jerzy

Inhaltsverzeichnis

Two Types of Electro-Elastic Coupling and Their Role in Properties of Line Defects in Unbounded Anisotropic Media.- Piezoelectricity and Piezomagnetism: Basic Concepts and Equations.- Mindlin’s Electro-Elastic Coupling due to Polarization Gradient.- General Electro-Elastic Line Defect in Unbounded Piezoelectric Body.- Thermo-Electro-Elastic Fields Accompanying Plastic Deformation.- Some Extensions for Dislocations in Materials with Polarization Gradient.- 1D and 2D Electro-Elastic Coupled Fields in Media with Surfaces and Interfaces.- Coupled Fields of Thermal Inclusion in Media with Polarization Gradient.- Green’s Functions for Piezoelectric Strip with a General Line Source.- Green’s Functions for Piezoelectric Strip with Line Surface Sources.- 2D Electro-Elastic Fields in a Piezoelectric Layer-Substrate Structure.- Acoustic Waves in Piezornagnetic and Piezoelectric Structures.

Leseproben

"7 GREENS FUNCTIONS FOR PIEZOELECTRIC STRIP WITH A GENERAL LINE SOURCE (p. 125-126)

In this chapter we are going to derive the static Green function describing the 2D coupled fields in arbitrary piezoelectric strip excited by a general line defect parallel to the surfaces and consisting of the four line sources introduced in Sec. 3.3 (c): the line of forces f, the line of charge q, the straight dislocation with the Burgers vector b, and its electrostatic analog of the strength A(p. As we have seen in Ch. 3, the latter line defect is completely determined by the discontinuity Aip in the electrical potential across the arbitrary plane cut ending on the line, which in our case determines the coinciding positions of all the mentioned sources.

The first studies in this field were accomplished for a particular case of straight dislocations in isotropic elastic plates [55-59]. These results were later extended for anisotropic [53] and possibly inhomogeneous [54] purely elastic (nonpiezoelectric) infinite strips. The further extension of the theory for the case of arbitrary piezoelectric strips has been developed in our paper [28]. The content of Chapter 7 is based on this paper.

7.1 Statement of the problem and basic equations

(a) Some preliminary remarks

The aim of this chapter is a derivation of the electro-elastic fields excited in a piezoelectric plate by the general line defect defined above. Of course, such an object, as the general line defect first introduced by Lothe & Barnett [63], is only conventionally a "defect", because among its four constituent line sources there is only one lattice defect - the dislocation. So, perhaps, it would be more correct to talk about the general line source rather than about a defect.

Anyway, independently of the terminology introduced and accepted before us, below we are going to find the physical fields excited by such a combined source. In our analysis it will be convenient to follow the method developed in [54] for purely elastic anisotropic continuously layered media, specifying the problem to a homogeneous medium and simultaneously extending it for a piezoelectric case. Such an extension turns out to be not quite straightforward because of the electrical boundary conditions, which are determined by a continuity of the normal component of electric displacement on the interfaces between the strip and the adjoined isotropic dielectric media. Our consideration will be based on the Stroh-like approach presented in details in Chapter 3 (Sec. 3.3 (c)) where the problem was already formulated for the same general line defect in unbounded medium."