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1996 | Buch

Thermoelastic Deformations

verfasst von: D. Ieşan, A. Scalia

Verlag: Springer Netherlands

Buchreihe : Solid Mechanics and Its Applications

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Über dieses Buch

The theory of thermoelasticity studies the interaction between thermal and mechan­ ical fields in elastic bodies. This theory is of interest both for the mathematical and technical point of view. Intense interest has been shown recently in this field owing to the great practical importance of dynamical effects in aeronautics, nu­ clear reactors, and its potential importance in cryogenic applications. This work is concerned mainly with basic problems of the theory of thermoelasticity. Ther­ moelasticity of polar materials and the theories of thermoelasticity with finite wave speeds are not considered here. The reader interested in these subjects will find a full account in the works of Nowacki [280], Chandrasekharaiah [60] and Ignaczak [195]. Our purpose in this work is to present a systematic treatment of some results established in the theory of thermoelasticity. On the whole, the subject matter is directed towards recent developments. Chapter 1 is concerned mainly with the development of the fundamental equa­ tions of the theory of thermoelasticity. The kinematics and primitive concepts associated with the basic principles are developed and emphasized only to the ex­ tent that they are needed in our treatment of the subject. Chapter 2 is devoted to a study of linear thermoelastic deformations for prestressed bodies. We have at­ tempted to isolate those conceptual and mathematical difficulties which arise over and above those inherent in the problems concerned with unstressed bodies.

Inhaltsverzeichnis

Frontmatter
1. The Foundations of the Theory of Thermoelasticity
Abstract
We consider a body that at time t 0 occupies the region B 0 of Euclidean three-dimensional space E 3. Throughout this book, unless specified to the contrary, B 0 will denote a bounded regular region in the sense of Kellogg. The configuration of the body at time t 0 is taken as the reference configuration. The motion of the body is referred to the reference configuration and a fixed system of rectangular Cartesian axes. Let B 0 be at rest relative to the considered system of axes. We identify a typical particle X of the body with its position X in the reference configuration. The coordinates of a typical particle X in B 0 are X A (A = 1, 2, 3). The coordinates of this particle in the position x at time t are denoted by x i .
D. Ieşan, A. Scalia
2. The Linear Theory of Thermoelasticity for Bodies with Initial Stress and Initial Heat Flux
Abstract
In what follows we establish the equations governing infinitesimal thermoelastic deformations superimposed on large deformations. The theory of infinitesimal thermoelastic deformations in a body which has already been subjected to an isothermal elastic deformation was established by England and Green [120] and Green [149]. The equations established in [120], [149] have been employed by Knops and Wilkes [223], p. 187 in a discussion of thermoelastic stability. The theory of infinitesimal thermoelastic deformations superimposed on a large deformation at nonconstant temperature was established by Iesan [182].
D. Ieşan, A. Scalia
3. Thermoelastodynamics of Bodies without Initial Deformations
Abstract
In what follows we assume that the primary state is identical with that of the initial body B 0. Moreover, we suppose that the primary state is a configuration of equilibrium at the constant temperature T 0 and without stresses.
D. Ieşan, A. Scalia
4. Problems of Equilibrium
Abstract
In this chapter, we consider the equilibrium theory of classical thermoelasticity. In the absence of time dependence, the basic equations from Section 3.1 reduce to the equations of equilibrium
(4.1.1)
the equilibrium energy equation
(4.1.2)
the constitutive equations
(4.1.3)
(4.1.4)
and the geometrical equations
(4.1.5)
on B. The constitutive coefficients satisfy the properties (3.1.4).
D. Ieşan, A. Scalia
5. Nonlinear Thermoelasticity
Abstract
In this section we consider the equations of the nonlinear theory of thermoelastodynamics. In [92], Dafermos has established the continuous dependence of smooth thermodynamic processes upon the initial state and supply terms for nonconductors of heat. The results of Dafermos have been extended by Chirita [69] to heat-conducting elastic bodies. This section is devoted to the continuous dependence results given in [92], [69].
D. Ieşan, A. Scalia
Backmatter
Metadaten
Titel
Thermoelastic Deformations
verfasst von
D. Ieşan
A. Scalia
Copyright-Jahr
1996
Verlag
Springer Netherlands
Electronic ISBN
978-94-017-3517-9
Print ISBN
978-90-481-4752-6
DOI
https://doi.org/10.1007/978-94-017-3517-9