Fundamentals of the Theory of Plasticity
eBook - ePub

Fundamentals of the Theory of Plasticity

  1. 512 pages
  2. English
  3. ePUB (mobile friendly)
  4. Available on iOS & Android
eBook - ePub

Fundamentals of the Theory of Plasticity

About this book

Based on the author's series of lectures at the Mechanics-Mathematics Faculty of the University of Leningrad, this text is primarily concerned with the plastic deformation of metals at normal temperatures, as applied to the strength of machines and structures. Its focus on delivering a simple presentation of the basic equations of plasticity theory encompasses the best-developed methods for solving the equations; it also considers problems associated with the special nature of plastic state and the most important engineering applications of plasticity theory.
This volume traces the main trends in the theory's development, assuming readers' familiarity with the fundamentals of strength of materials and elasticity theory. Advanced topics are marked with an asterisk and can be omitted on a first reading. Intended as a text for advanced engineering students, as well as a reference book for practicing engineers, it features problems at the end of each chapter that enable readers to test their grasp of the material.
Contents include the fundamentals of continuum mechanics, equations of plastic state and elastic-plastic equilibrium, torsion, plane strain and stress, and axially symmetric strain. Additional topics range from extremum principles and energy methods of solution to theory of shakedown, stability of elastic-plastic equilibrium, dynamic problems, complex media, and viscoplasticity. An extensive bibliography appears at the end of the book. 1971 edition.

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Yes, you can access Fundamentals of the Theory of Plasticity by L. M. Kachanov in PDF and/or ePUB format, as well as other popular books in Technology & Engineering & Civil Engineering. We have over one million books available in our catalogue for you to explore.

1

Basic Concepts in the Mechanics of Continuous Media

In this chapter we outline the basic formulae of the theory of stress and strain; in the process we identify the most important information for the development of the theory of plasticity.

§1. Stress

1.1. Stress

At a given point in a continuous medium the state of stress is characterized by a symmetric stress tensor
e9780486150826_i0007.webp
(1.1)
where σx, σy, σz are the normal components, and τxy, τyz, τxz the tangential components of stress in a rectangular coordinate system with axes x, y, z.
The stress vector p on an arbitrarily oriented surface with unit normal n (fig. 1) is given by Cauchy’s formulae:
e9780486150826_i0008.webp
(1.2)
where nx, ny, nz are the components of the unit normal n and are equal respectively to the direction cosines cos (n, x), cos (n, y), cos (n, z).
e9780486150826_i0009.webp
Fig. 1.
The projection of the vector p in the direction of the normal gives the normal stress σn, acting on the surface in question:
e9780486150826_i0010.webp
(1.3)
The magnitude of the tangential stress τn equals
e9780486150826_i0011.webp
(1.4)
At each point of the medium there exist three mutually perpendicular surface elements on which the tangential stresses are zero. The directions of the normals to these surfaces constitute the principal directions of the stress tensor and do not depend on the choice of the coordinate system x, y, z. This means that any stress state at the given point may be induced by stretching the neighbourhood of the point in three mutually perpendicular directions. The corresponding stresses are called principal normal stresses; we shall denote them by σ1, σ2, σ3 and number the principal axes so that
e9780486150826_i0012.webp
(1.5)
The stress tensor, referred to principal axes, has the form
e9780486150826_i0013.webp
e9780486150826_i0014.webp
Fig. 2.
It is not difficult to show from formulae (1.2)−(1.4) that in cross-sections, which bisect the angles between the principal planes and pass respectively through the principal axes 1, 2, 3 (fig. 2), the tangential stresses have magnitudes
e9780486150826_i0015.webp
The tangential stresses on these cross-sections have extremum values and are called principal tangential stresses. We define these by the formulae
e9780486150826_i0016.webp
(1.6)
With change in the orientation of a surface, the intensity of the tangential stress τn acting on it also changes. The maximum value of τn at a given point is called the maximum tangential stress τmax. If condition (1.5) is satisfied, then
τmax = −τ2.
I...

Table of contents

  1. DOVER BOOKS ON ENGINEERING
  2. Title Page
  3. Copyright Page
  4. Table of Contents
  5. Preface to the Second Edition
  6. Basic Notation
  7. Errata
  8. Introduction
  9. 1 - Basic Concepts in the Mechanics of Continuous Media
  10. 2 - Equations of the Plastic State
  11. 3 - Equations of Elastic-Plastic Equilibrium. The Simplest Problems
  12. 4 - Torsion
  13. 5 - Plane Strain
  14. 6 - Plane Stress
  15. 7 - Axisymmetric Strain
  16. 8 - Extremum Principles and Energy Methods
  17. 9 - Theory of Shakedown
  18. 10 - Stability of Elastic-Plastic Equilibrium
  19. 11 - Dynamical Problems
  20. 12 - Composite Media. Visco-Plasticity
  21. Appendix
  22. Bibliography)
  23. Subject Index