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The theory of elasticity is concerned with the mechanics of deformable media which, after the removal of the forces producing deformation, completely recover their original shape and give up all the work expended in the deformation.
The first attempts to develop the theory of elasticity on the basis of the concept of a continuous medium, which enables one to ignore its molecular structure and describe macroscopic phenomena by the methods of mathematical analysis, date back to the first half of the eighteenth century.
The fundamental contribution to the classical theory was made by R. Hooke, C. L. M. H. Navier, A. L. Cauchy, G. Lame, G. Green, B. P. E. Clapeyron. In 1678 Hooke established a law linearly con- necting stresses and strains.
After Navier established the basic equations in 1821 and Cauchy developed the theory of stress and strain, of great importance in the development of elasticity theory were the investigations of B. de Saint Venant. In his classical work on the theory of torsion and bending Saint Venant gave the solution of the problems of torsion and bending of prismatic bars on the basis of the general equations of the theory of elasticity. In these investigations Saint Venant devised a semi-inverse method for the solution of elasticity problems, formulated the famous Saint Venant’s principle, which enables one to obtain the solution of elasticity problems. Since then much effort has been made to develop the theory of elasticity and its applications, a number of general theorems have been proved, the general methods for the integration of differential equations of equilibrium and motion have been proposed, many special problems of fundamental interest have been solved. The development of new fields of engineering demands deeper and more extensive studies of the theory of elasticity. High velocities call for the formulation and solution of complex vibrational problems. Lightweight metallic structures draw particular attention to the question of elastic stability. The concentration of stress entails dangerous consequences, which cannot safely be ignored.
Contents
Notation 9
Introduction 13
Chapter I. ELEMENTS OF TENSOR CALCULUS 15
- Scalars, Vectors, and Tensors 16
- Addition, Multiplication, and Contraction of Tensors. The Quotient Law of Tensors 19
- The Metric Tensor 22
- Differentiation of Base Vectors. The Christoffel Symbols 28
- A Parallel Field of Vectors 30
- The Riemann-Christoffel Tensor. Derivative of a Veetor. The Gauss-Ostrogradsky Formula. The 𝜀-tensor 32
Chapter II. THEORY OF STRESS 39
- Types of External Forces 39
- The Method of Sections. The Stress Vector 41
- The Stress Tensor 43
- Equations of Motion and Equilibrium in Terms of the Components of the Stress Tensor 44
- Surface Conditions 47
- Equations of Motion and Equilibrium Referred to a Cartesian Co-ordinate System 48
- Equations of Motion and Equilibrium Referred to Cylindrical and Spherical Co-ordinates 49
- Determination of the Principal Normal Stresses 52
Chapter III. THEORY OF STRAIN 55
- The Finite Strain Tensor 55
- The Small Strain Tensor 59
- Strai Compatibility Equations 60
- The Strain Tensor Referred to a Cartesian Co-ordinate System 61
- Components of the Small Strain and Rotation Tensors Referred to Cylindrical and Spherical Co-ordinates 62
- Principal Extensions 64
- Strain Compatibility Equations in Some Co-ordinate Systems (Saint Venant’s Conditions) 65
- Determination of Displacements from the Components of the Small Strain Tensor 66
Chapter IV. STRESS-STRAIN RELATIONS 69
- Generalized Hooke’s Law 69
- Work Done by External Forces 70
- Stress Tensor Potential 71
- Potential in the Case of a Linearly Elastic Body 75
- Various Cases of Elastic Symmetry of a Body 75
- Thermal Stresses 80
- A Energy Integral for the Equations of Motion of an Elastic Body 80
- Betti’s Identity 82
- Clapeyron’s Theorem 82
Chapter V. COMPLETE SYSTEM OF FUNDAMENTAL EQUATIONS IN THE THEORY OF ELASTICITY 84
- Equations of Elastic Equilibrium and Motion in Terms of Displacements 84
- Equations in Terms of Stress Components 90
- Fundamental Boundary Value Problems in Elastostatics. Uniqueness of Solution 93
- Fundamental Problems in Elastodynamics 95
- Saint Venant’s Principle (Principle of Softening of Boundary Conditions) 96
- Direct and Inverse Solutions of Elasticity Problems. Saint Venant’s Semi-inverse Method 98
- Simple Problems of the Theory of Elasticity 99
Chapter VI. THE PLANE PROBLEM IN THE THEORY OF ELASTICITY 108
- Plane Strain 108
- Plane Stress 111
- Generalized Plane Stress 113
- Airy’s Stress Function 115
- Airy’s Function in Polar Co-ordinates. Lamé’s Problem 120
- Complex Representation of a Biharmonic Function, of the Components of the Displacement Vector and the Stress Tensor 127
- Degree of Determinancy of the Introduced Functions and Restrictions Imposed on Them 132
- Fundamental Boundary Value Problems and Their Reduction to Problems of Complex Function Theory 138
- Maurice Lévy’s Theorem 141
- Conformal Mapping Method 142
- Cauchy-type Integral 145
- Harnack’s Theorem 151
- Riemann Boundary Value Problem 151
- Reduction of the Fundamental Boundary Value Problems to Functional Equations 154
- Equilibrium of a Hollow Circular Cylinder 155
- Infinite Plate with an Elliptic Hole 159
- Solution of Boundary Value Problems for a Half-plane 164
- Some Information on Fourier Integral Transformation 170
- Infinite Plane Deformed Under Body Forces 174
- Solution of the Biharmonic Equation for a Weightless Half-plane 177
Chapter VII. TORSION AND BENDING OF PRISMATIC BODIES 182
- Torsion of a Prismatic Body of Arbitrary Simply Connected Cross Section 182
- Some Properties of Shearing Stresses 187
- Torsion at Hollow Prismatic Bodies 188
- Shear Circulation Theorem 190
- Analogies in Torsion 191
- Complex Torsion Function 196
- Solution of Special Torsion Problems 198
- Bending of a Prismatic Body Fixed at One End 206
- The Centre of Flexure 211
- Bending of a Prismatic Body of Elliptical Cross Section 216
Chapter VIII. GENERAL THEOREMS OF THE THEORY OF ELASTICITY. VARIATIONAL METHODS 219
- Betti’s Reciprocal Theorem 219
- Principle of Minimum Potential Energy 220
- Principle of Minimum Complementary Work—Castigliano’s Principle 222
- Rayleigh-Ritz Method 224
- Reissner’s Variational Principle 228
- Equilibrium Equations and Boundary Conditions for a Geometrically Non-linear Body 230
Chapter IX. THREE-DIMENSIONAL STATIC PROBLEMS 232
- Kelvin’s and the Boussinesq-Papkovich Solutions 232
- Doursinesa’s Elementary Solutions of the First and Second Kind 236
- Pressure on the Surface of a Semi-infinite Body 238
- Hertz’s Problem of the Pressure Between Two Bodies in Contact 240
- Symmetrical Deformation of a Bedy of Revolution 246
- Thermal Stresses 256
Chapter X. THEORY OF PROPAGATION OF ELASTIC WAVES 258
- Two Types of Waves 258
- Rayleigh Surface Waves 262
- Love Waves 265
Chapter XI. THEORY OF THIN PLATES 268
- Differential Equation for Bending of Thin Plates 268
- Boundary Conditions 271
- Bending Equation for a Plate Referred to Polar Co-ordinates 274
- Symmetrical Bending of a Circular Plate 276
Literature 278
Subject Index 279