Structural analysis with applications to aerospace structures

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Structural Analysis
SOLID MECHANICS AND ITS APPLICATIONS
Volume 163
Series Editor: G.M.L. GLADWELL
Department of Civil Engineering
University of Waterloo
Waterloo, Ontario, Canada N2L 3GI
Aims and Scope of the Series
The fundamental questions arising in mechanics are: Why?, How?, and How much?
The aim of this series is to provide lucid accounts written by authoritative research-
ers giving vision and insight in answering these questions on the subject of mech-
anics as it relates to solids.
The scope of the series covers the entire spectrum of solid mechanics. Thus it in-
cludes the foundation of mechanics; variational formulations; computational mech-
anics; statics, kinematics and dynamics of rigid and elastic bodies: vibrations of
solids and structures; dynamical systems and chaos; the theories of elasticity, plas-
ticity and viscoelasticity; composite materials; rods, beams, shells and membranes;
structural control and stability; soils, rocks and geomechanics; fracture; tribology;
experimental mechanics; biomechanics and machine design.
The median level of presentation is the first year graduate student. Some texts are
monographs defining the current state of the field; others are accessible to final year
undergraduates; but essentially the emphasis is on readability and clarity.
For other titles published in this series, go to
www.springer.com/series/6557
O.A. Bauchau • J.I. Craig
Structural Analysis
With Applications to Aerospace Structures
O.A. Bauchau J.I. Craig
School of Aerospace Engineering School of Aerospace Engineering
Georgia Institute of Technology Georgia Institute of Technology
Atlanta, Georgia Atlanta, Georgia
USA USA
Printed on acid-free paper
© Springer Science + Business Media B.V. 2009
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Library of Congress Control Number: 2009932893
ISBN 978-90-481-2515-9 e-ISBN 978-90-481-2516-6
To our wives, Yi-Ling and Nancy, and our families
Preface
Engineered structures are almost as old as human civilization and undoubtedly began
with rudimentary tools and the first dwellings outside caves. Great progress has been
made over thousands of years, and our world is now filled with engineered struc-
from fragile human-powered aircraft to sleek jets and thundering rockets are, in our
opinion, among the most challenging and creative examples of these efforts.
The study of mechanics and structural analysis has been an important area of en-
gineering over the past 300 years, and some of the greatest minds have contributed
to its development. Newton formulated the most basic principles of equilibrium in
the 17th century, but fundamental contributions have continued well into the 20th
century. Today, structural analysis is generally considered to be a mature field with
well-established principles and practical tools for analysis and design. A key rea-
son for this is, without doubt, the emergence of the finite element method and its
widespread application in all areas of structural engineering. As a result, much of
today’s emphasis in the field is no longer on structural analysis, but instead is on the
use of new materials and design synthesis.
The field of aerospace structural analysis began with the first attempts to build
flying machines, but even today, it is a much smaller and narrower field treated in far
fewer textbooks as compared to the fields of structural analysis in civil and mechan-
ical engineering. Engineering students have access to several excellent texts such as
those by Donaldson [1] and Megson [2], but many other notable textbooks are now
out of print.
This textbook has emerged over the past two decades from our efforts to teach
in aerospace engineering. By the time students enroll in the undergraduate course,
they have studied statics and covered introductory mechanics of deformable bodies
dealing primarily with beam bending. These introductory courses are taught using
texts devoted largely to applications in civil and mechanical engineering, leaving
our students with little appreciation for some of the unique and challenging features
of aerospace structures, which often involve thin-walled structures made of fiber-
reinforced composite materials. In addition, while in widespread use in industry and
tures from nano-scale machines to soaring buildings. Aerospace structures ranging
core courses in advanced structural analysis to undergraduate and graduate students
VIII Preface
the subject of numerous specialized textbooks, the finite element method is only
slowly finding its way into general structural analysis texts as older applied methods
and special analysis techniques are phased out.
The book is divided into four parts. The first part deals with basic tools and
concepts that provide the foundation for the other three parts. It begins with an intro-
duction to the equations of linear elasticity, which underlie all of structural analysis.
A second chapter presents the constitutive laws for homogeneous, isotropic and lin-
early elastic material but also includes an introduction to anisotropic materials and
particularly to transversely isotropic materials that are typical of layered composites.
The first part concludes with chapter 4, which defines isostatic and hyperstatic prob-
lems and introduces the fundamental solution procedures of structural analysis: the
displacement method and the force method.
Part 2 develops Euler-Bernoulli beam theory with emphasis on the treatment of
beams presenting general cross-sectional configurations. Torsion of circular cross-
sections is discussed next, along with Saint-Venant torsion theory for bars of arbitrary
shape. A lengthy chapter is devoted to thin-walled beams typical of those used in
aerospace structures. Coupled bending-twisting and nonuniform torsion problems
are also addressed.
Part 3 introduces the two fundamental principles of virtual work that are the ba-
sis for the powerful and versatile energy methods. They provide tools to treat more
realistic and complex problems in an efficient manner. A key topic in Part 3 is the de-
velopment of methods to obtain approximate solution for complex problems. First,
the Rayleigh-Ritz method is introduced in a cursory manner; next, applications of
the weak statement of equilibrium and of energy principles are presented in a more
formal manner; finally, the finite element method applied to trusses and beams is
presented. Part 3 concludes with a formal introduction of variational methods and
general statements of the energy principles introduced earlier in more applied con-
texts.
Part 4 covers a selection of advanced topics of particular relevance to aerospace
structural analysis. These include introductions to plasticity and thermal stresses,
buckling of beams, shear deformations in beams and Kirchhoff plate theory.
In our experience, engineering students generally grasp concepts more quickly
when presented first with practical examples, which then lead to broader generaliza-
tions. Consequently, most concepts are first introduced by means of simple examples;
more formal and abstract statements are presented later, when the student has a better
grasp of the significance of the concepts. Furthermore, each chapter provides numer-
ous examples to demonstrate the application of the theory to practical problems.
Some of the examples are re-examined in successive chapters
to illustrate alternative
or more versatile solution methods. Step-by-step descriptions of important solution
procedures are provided.
As often as possible, the analysis of structural problems is approached in a unified
manner. First, kinematic assumptions are presented that describe the structure’s dis-
placement field in an approximate manner; next, the strain field is evaluated based on
the strain-displacement relationships; finally, the constitutive laws lead to the stress
field for which equilibrium equations are then established. In our experience, this ap-
Preface IX
proach reduces the confusion that students often face when presented with develop-
ments that don’t seem to follow any obvious direction or strategy but yet, inevitably
lead to the expected solution.
The topics covered in parts 1 and 2 along with chapters 9 and 10 from part 3 form
the basis for a four semester-hour course in advanced aerospace structural analysis
taught to junior and senior undergraduate students. An introductory graduate level
course covers part 2 and selected chapters in parts 3 and 4, but only after a brief
review of the material in part 1. A second graduate level course focusing on varia-
tional end energy methods covers part 3 and selected chapters in part 4. A number
of homework problems are included throughout these chapters. Some are straightfor-
ward applications of simple concepts, others are small projects that require the use of
computers and mathematical software, and others involve conceptual questions that
are more appropriate for quizzes and exams.
A thorough study of differential calculus including a basic treatment of ordinary
and partial differential equations is a prerequisite. Additional topics from linear al-
gebra and differential geometry are needed, and these are reviewed in an appendix.
Notation is a challenging issue in structural analysis. Given the limitations of
the Latin and Greek alphabets, the same symbols are sometimes used for different
purposes, but mostly in different contexts. Consequently, no attempt has been made
to provide a comprehensive list of symbols, which would lead to even more confu-
sion. Also, in mechanics and structural analysis, sign conventions present a major
hurdle for all students. To ease this problem, easy to remember sign conventions are
used systematically. Stresses and force resultants are positive on positive faces when
acting along positive coordinate directions. Moments and torques are positive on
positive faces when acting about positive coordinate directions using the right-hand
rule.
In a few instances, new or less familiar terms have been chosen because of their
importance in aerospace structural analysis. For instance, the terms “isostatic” and
“hyperstatic” structures are used to describe statically determinate and indetermi-
nate structures, respectively, because these terms concisely define concepts that often
puzzle and confuse students. Beam bending stiffnesses are indicated with the symbol
“H” rather than the more common “EI .” When dealing exclusively with homoge-
neous material, notation “EI” is easy to understand, but in presence of heteroge-
neous composite materials, encapsulating the spatially varying elasticity modulus in
the definition of the bending stiffness is a more rational approach.
It is traditional to use a bold typeface to represent vectors, arrays, and matri-
ces, but this is very difficult to reproduce in handwriting, whether in a lecture or in
personal notes. Instead, we have adopted a notation that is more suitable for hand-
written notes. Vectors and arrays are denoted using an underline, such as u or F . Unit
vectors are used frequently and are assigned a special notation using a single overbar,
such as ı¯1, which denotes the first Cartesian coordinate axis. We also use the over-
bar to denote non-dimensional scalar quantities, i.e., k¯ is a non-dimensional stiffness
coefficient. This is inconsistent, but the two uses are in such different contexts that
it should not lead to confusion. Matrices are indicated using a double-underline, i.e.,
C indicates a matrix of M rows and N columns.
X Preface
Finally, we are indebted to the many students at Georgia Tech who have given us
helpful and constructive feedback over the past decade as we developed the course
notes that are the predecessor of this book. We have tried to constructively utilize
their initial confusion and probing questions to clarify and refine the treatment of
important but confusing topics. We are also grateful for the many discussions and
valuable feedback from our colleagues, Profs. Erian Armanios, Sathya Hanagud,
Dewey Hodges, George Kardomateas, Massimo Ruzzene, and Virgil Smith, several
of whom have used our notes for teaching advanced aerospace structural analysis
here at Georgia Tech.
Atlanta, Georgia, Olivier Bauchau
July 2009 James Craig
Contents
Part I Basic tools and concepts
1 Basic equations of linear elasticity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
1.1 The concept of stress . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
1.1.1 The state of stress at a point . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
1.1.2 Volume equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . 7
1.1.3 Surface equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . 10
1.2 Analysis of the state of stress at a point . . . . . . . . . . . . . . . . . . . . . . . . 11
1.2.1 Stress components acting on an arbitrary face . . . . . . . . . . . . 11
1.2.2 Principal stresses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 13
1.2.3 Rotation of stresses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14
1.2.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
1.3 The state of plane stress . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
1.3.1 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
1.3.2 Stresses acting on an arbitrary face within the sheet . . . . . . . . 21
1.3.3 Principal stresses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22
1.3.4 Rotation of stresses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24
1.3.5 Special states of stress . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
1.3.6 Mohr’s circle for plane stress . . . . . . . . . . . . . . . . . . . . . . . . . . 27
1.3.7 Lame´’s ellipse . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 30
1.3.8 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31
1.4 The concept of strain . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33
1.4.1 The state of strain at a point . . . . . . . . . . . . . . . . . . . . . . . . . . . 34
1.4.2 The volumetric strain . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
1.5 Analysis of the state of strain at a point . . . . . . . . . . . . . . . . . . . . . . . . 38
1.5.1 Rotation of strains . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
1.5.2 Principal strains . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 40
1.6 The state of plane strain . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41
1.6.1 Strain-displacement relations for plane strain . . . . . . . . . . . . . 41
1.6.2 Rotation of strains . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42
XII Contents
1.6.3 Principal strains . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43
1.6.4 Mohr’s circle for plane strain . . . . . . . . . . . . . . . . . . . . . . . . . . 44
1.7 Measurement of strains . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
1.7.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49
1.8 Strain compatibility equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50
2 Constitutive behavior of materials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 53
2.1 Constitutive laws for isotropic materials . . . . . . . . . . . . . . . . . . . . . . . . 55
2.1.1 Homogeneous, isotropic, linearly elastic materials . . . . . . . . . 55
2.1.2 Thermal effects . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59
2.1.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61
2.1.4 Ductile materials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 63
2.1.5 Brittle materials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 65
2.2 Allowable stress . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 66
2.3 Yielding under combined loading . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 68
2.3.1 Tresca’s criterion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 68
2.3.2 Von Mises’ criterion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 70
2.3.3 Comparing Tresca’s and von Mises’ criteria . . . . . . . . . . . . . . 71
2.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 73
2.4 Material selection for structural performance . . . . . . . . . . . . . . . . . . . . 73
2.4.1 Strength design . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74
2.4.2 Stiffness design . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74
2.4.3 Buckling design . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75
2.5 Composite materials . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 76
2.5.1 Basic characteristics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 76
2.5.2 Stress diffusion in composites . . . . . . . . . . . . . . . . . . . . . . . . . . 78
2.6 Constitutive laws for anisotropic materials . . . . . . . . . . . . . . . . . . . . . . 82
2.6.1 Constitutive laws for a lamina in the fiber aligned triad . . . . . 85
2.6.2 Constitutive laws for a lamina in an arbitrary triad . . . . . . . . . 87
2.7 Strength of a transversely isotropic lamina . . . . . . . . . . . . . . . . . . . . . . 94
2.7.1 Strength of a lamina under simple loading conditions . . . . . . 94
2.7.2 Strength of a lamina under combined loading conditions . . . 95
2.7.3 The Tsai-Wu failure criterion . . . . . . . . . . . . . . . . . . . . . . . . . . 96
2.7.4 The reserve factor . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 98
3 Linear elasticity solutions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 101
3.1 Solution procedures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 102
3.1.1 Displacement formulation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 103
3.1.2 Stress formulation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 103
3.1.3 Solutions to elasticity problems . . . . . . . . . . . . . . . . . . . . . . . . 104
3.2 Plane strain problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 110
3.3 Plane stress problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 111
3.4 Plane strain and plane stress in polar coordinates . . . . . . . . . . . . . . . . 113
3.5 Problem featuring cylindrical symmetry . . . . . . . . . . . . . . . . . . . . . . . . 116
3.5.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 133
Contents XIII
4 Engineering structural analysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 137
4.1 Solution approaches . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 137
4.2 Bar under constant axial force . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 138
4.3 Hyperstatic systems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 144
4.3.1 Solution procedures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 145
4.3.2 The displacement or stiffness method . . . . . . . . . . . . . . . . . . . 146
4.3.3 The force or flexibility method . . . . . . . . . . . . . . . . . . . . . . . . . 151
4.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 156
4.3.5 Thermal effects in hyperstatic system . . . . . . . . . . . . . . . . . . . 157
4.3.6 Manufacturing imperfection effects in hyperstatic system . . . 161
4.3.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 164
4.4 Pressure vessels . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 165
4.4.1 Rings under internal pressure . . . . . . . . . . . . . . . . . . . . . . . . . . 165
4.4.2 Cylindrical pressure vessels . . . . . . . . . . . . . . . . . . . . . . . . . . . 166
4.4.3 Spherical pressure vessels . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 167
4.4.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 168
4.5 Saint-Venant’s principle . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 169
Part II Beams and thin-wall structures
5 Euler-Bernoulli beam theory . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 173
5.1 The Euler-Bernoulli assumptions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 174
5.2 Implications of the Euler-Bernoulli assumptions . . . . . . . . . . . . . . . . . 175
5.3 Stress resultants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 177
5.4 Beams subjected to axial loads . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 178
5.4.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 179
5.4.2 Sectional constitutive law . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 179
5.4.3 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 180
5.4.4 Governing equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 181
5.4.5 The sectional axial stiffness . . . . . . . . . . . . . . . . . . . . . . . . . . . . 182
5.4.6 The axial stress distribution . . . . . . . . . . . . . . . . . . . . . . . . . . . . 182
5.4.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 185
5.5 Beams subjected to transverse loads . . . . . . . . . . . . . . . . . . . . . . . . . . . 186
5.5.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 186
5.5.2 Sectional constitutive law . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 187
5.5.3 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 188
5.5.4 Governing equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 189
5.5.5 The sectional bending stiffness . . . . . . . . . . . . . . . . . . . . . . . . . 191
5.5.6 The axial stress distribution . . . . . . . . . . . . . . . . . . . . . . . . . . . . 193
5.5.7 Rational design of beams under bending . . . . . . . . . . . . . . . . . 194
5.5.8 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 211
5.6 Beams subjected to combined axial and transverse loads . . . . . . . . . . 217
5.6.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 217
5.6.2 Sectional constitutive
law . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 217
XIV Contents
5.6.3 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 218
5.6.4 Governing equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 219
6 Three-dimensional beam theory . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 223
6.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 224
6.2 Sectional constitutive law . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 225
6.3 Sectional equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 227
6.4 Governing equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 229
6.5 Decoupling the three-dimensional problem . . . . . . . . . . . . . . . . . . . . . 230
6.5.1 Definition of the principal axes of bending . . . . . . . . . . . . . . . 231
6.5.2 Decoupled governing equations . . . . . . . . . . . . . . . . . . . . . . . . 232
6.6 The principal centroidal axes of bending . . . . . . . . . . . . . . . . . . . . . . . 233
6.6.1 The bending stiffness ellipse . . . . . . . . . . . . . . . . . . . . . . . . . . . 235
6.7 The neutral axis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 236
6.8 Evaluation of sectional stiffnesses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 240
6.8.1 The parallel axis theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 240
6.8.2 Thin-walled sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 242
6.8.3 Triangular area equivalence method . . . . . . . . . . . . . . . . . . . . . 243
6.8.4 Useful results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 244
6.8.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 247
6.9 Summary of three-dimensional beam theory . . . . . . . . . . . . . . . . . . . . 248
6.9.1 Discussion of the results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 255
6.10 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 255
7 Torsion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 261
7.1 Torsion of circular cylinders . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 261
7.1.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 262
7.1.2 The stress field . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 264
7.1.3 Sectional constitutive law . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 265
7.1.4 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 266
7.1.5 Governing equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 266
7.1.6 The torsional stiffness . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 267
7.1.7 Measuring the torsional stiffness . . . . . . . . . . . . . . . . . . . . . . . 267
7.1.8 The shear stress distribution . . . . . . . . . . . . . . . . . . . . . . . . . . . 268
7.1.9 Rational design of cylinders under torsion . . . . . . . . . . . . . . . 270
7.1.10 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 271
7.2 Torsion combined with axial force and bending moments . . . . . . . . . 271
7.2.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 274
7.3 Torsion of bars with arbitrary cross-sections . . . . . . . . . . . . . . . . . . . . 275
7.3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 275
7.3.2 Saint-Venant’s solution . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 276
7.3.3 Saint-Venant’s solution for a rectangular cross-section . . . . . 284
7.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 289
7.4 Torsion of a thin rectangular cross-section . . . . . . . . . . . . . . . . . . . . . . 290
7.5 Torsion of thin-walled open sections . . . . . . . . . . . . . . . . . . . . . . . . . . . 292
Contents XV
7.5.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 294
8 Thin-walled beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 297
8.1 Basic equations for thin-walled beams. . . . . . . . . . . . . . . . . . . . . . . . . . 297
8.1.1 The thin wall assumption . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 297
8.1.2 Stress flows . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 298
8.1.3 Stress resultants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 299
8.1.4 Sign conventions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 301
8.1.5 Local equilibrium equation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 302
8.2 Bending of thin-walled beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 303
8.2.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 304
8.3 Shearing of thin-walled beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 307
8.3.1 Shearing of open sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 308
8.3.2 Evaluation of stiffness static moments . . . . . . . . . . . . . . . . . . . 308
8.3.3 Shear flow distributions in open sections . . . . . . . . . . . . . . . . . 309
8.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 317
8.3.5 Shear center for open sections . . . . . . . . . . . . . . . . . . . . . . . . . . 318
8.3.6 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 324
8.3.7 Shearing of closed sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . 325
8.3.8 Shearing of multi-cellular sections . . . . . . . . . . . . . . . . . . . . . . 329
8.3.9 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 332
8.4 The shear center . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 334
8.4.1 Calculation of the shear center location . . . . . . . . . . . . . . . . . . 334
8.4.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 341
8.5 Torsion of thin-walled beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 343
8.5.1 Torsion of open sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 343
8.5.2 Torsion of closed section . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 343
8.5.3 Comparison of open and closed sections . . . . . . . . . . . . . . . . . 345
8.5.4 Torsion of combined open and closed sections . . . . . . . . . . . . 346
8.5.5 Torsion of multi-cellular sections . . . . . . . . . . . . . . . . . . . . . . . 347
8.5.6 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 351
8.6 Coupled bending-torsion problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . 354
8.6.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 361
8.7 Warping of thin-walled beams under torsion . . . . . . . . . . . . . . . . . . . . 362
8.7.1 Kinematic description . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 362
8.7.2 Stress-strain relations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 363
8.7.3 Warping of open sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 364
8.7.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
. . . . . . . . . 369
8.7.5 Warping of closed sections . . . . . . . . . . . . . . . . . . . . . . . . . . . . 369
8.7.6 Warping of multi-cellular sections . . . . . . . . . . . . . . . . . . . . . . 371
8.8 Equivalence of the shear and twist centers . . . . . . . . . . . . . . . . . . . . . . 371
8.9 Non-uniform torsion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 372
8.9.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 376
8.10 Structural idealization . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 377
8.10.1 Sheet-stringer approximation of a thin-walled section . . . . . . 378
XVI Contents
8.10.2 Axial stress in the stringers . . . . . . . . . . . . . . . . . . . . . . . . . . . . 381
8.10.3 Shear flow in the sheet components . . . . . . . . . . . . . . . . . . . . . 381
8.10.4 Torsion of sheet-stringer sections . . . . . . . . . . . . . . . . . . . . . . . 384
8.10.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 390
Part III Energy and variational methods
9 Virtual work principles . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 395
9.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 395
9.2 Equilibrium and work fundamentals . . . . . . . . . . . . . . . . . . . . . . . . . . . 396
9.2.1 Static equilibrium conditions . . . . . . . . . . . . . . . . . . . . . . . . . . 396
9.2.2 Concept of mechanical work . . . . . . . . . . . . . . . . . . . . . . . . . . . 399
9.3 Principle of virtual work . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 400
9.3.1 Principle of virtual work for a single particle . . . . . . . . . . . . . 400
9.3.2 Kinematically admissible virtual displacements . . . . . . . . . . . 405
9.3.3 Use of infinitesimal displacements as virtual displacements . 410
9.3.4 Principle of virtual work for a system of particles . . . . . . . . . 412
9.4 Principle of virtual work applied to mechanical systems . . . . . . . . . . 415
9.4.1 Generalized coordinates and forces . . . . . . . . . . . . . . . . . . . . . 420
9.4.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 425
9.5 Principle of virtual work applied to truss structures . . . . . . . . . . . . . . 428
9.5.1 Truss structures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 428
9.5.2 Solution using Newton’s law . . . . . . . . . . . . . . . . . . . . . . . . . . . 431
9.5.3 Solution using kinematically admissible virtual displacements432
9.5.4 Solution using arbitrary virtual displacements . . . . . . . . . . . . 433
9.6 Principle of complementary virtual work . . . . . . . . . . . . . . . . . . . . . . . 437
9.6.1 Compatibility equations for a planar truss . . . . . . . . . . . . . . . . 438
9.6.2 Principle of complementary virtual work for trusses . . . . . . . 441
9.6.3 Complementary virtual work . . . . . . . . . . . . . . . . . . . . . . . . . . 445
9.6.4 Applications to trusses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 446
9.6.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 449
9.6.6 Unit load method for trusses . . . . . . . . . . . . . . . . . . . . . . . . . . . 449
9.6.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 455
9.7 Internal virtual work in beams and solids . . . . . . . . . . . . . . . . . . . . . . . 456
9.7.1 Beam bending . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 457
9.7.2 Beam twisting . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 458
9.7.3 Three-dimensional solid . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 459
9.7.4 Euler-Bernoulli beam . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 461
9.7.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 462
9.7.6 Unit load method for beams . . . . . . . . . . . . . . . . . . . . . . . . . . . 462
9.7.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 470
9.8 Application of the unit load method to hyperstatic problems . . . . . . . 472
9.8.1 Force method for trusses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 473
9.8.2 Force method for beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 480
Contents XVII
9.8.3 Combined truss and beam problems . . . . . . . . . . . . . . . . . . . . . 485
9.8.4 Multiple redundancies . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 487
9.8.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 489
10 Energy methods . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 493
10.1 Conservative forces . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 494
10.1.1 Potential for internal and external forces . . . . . . . . . . . . . . . . . 497
10.1.2 Calculation of the potential functions . . . . . . . . . . . . . . . . . . . . 498
10.2 Principle of minimum total potential energy . . . . . . . . . . . . . . . . . . . . 500
10.2.1 Non-conservative external forces . . . . . . . . . . . . . . . . . . . . . . . 503
10.3 Strain energy in springs . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 504
10.3.1 Rectilinear springs . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 504
10.3.2 Torsional springs . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 508
10.3.3 Bars . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 509
10.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 513
10.4 Strain energy in beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 514
10.4.1 Beam under axial loads . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 514
10.4.2 Beam under transverse loads . . . . . . . . . . . . . . . . . . . . . . . . . . . 515
10.4.3 Beam under torsional loads . . . . . . . . . . . . . . . . . . . . . . . . . . . . 516
10.4.4 Relationship with virtual work . . . . . . . . . . . . . . . . . . . . . . . . . 517
10.5 Strain energy in solids . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 519
10.5.1 Three-dimensional solid . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 519
10.5.2 Three-dimensional beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 520
10.6 Applications to trusses and beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 521
10.6.1 Applications to trusses . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 521
10.6.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 525
10.6.3 Applications to beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 527
10.7 Development of a finite element formulation for trusses . . . . . . . . . . 529
10.7.1 General description of the problem . . . . . . . . . . . . . . . . . . . . . 530
10.7.2 Kinematics of an element . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 531
10.7.3 Element elongation and force . . . . . . . . . . . . . . . . . . . . . . . . . . 533
10.7.4 Element strain energy and stiffness matrix . . . . . . . . . . . . . . . 533
10.7.5 Element external potential and load array . . . . . . . . . . . . . . . . 535
10.7.6 Assembly procedure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 535
10.7.7 Alternative description of the assembly procedure . . . . . . . . . 538
10.7.8 Derivation
of the governing equations . . . . . . . . . . . . . . . . . . . 539
10.7.9 Solution procedure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 540
10.7.10Solution procedure using partitioning . . . . . . . . . . . . . . . . . . . 542
10.7.11Post-processing . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 544
10.7.12Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 547
10.8 Principle of minimum complementary energy . . . . . . . . . . . . . . . . . . . 548
10.8.1 The potential of the prescribed displacements . . . . . . . . . . . . . 548
10.8.2 Constitutive laws for elastic materials . . . . . . . . . . . . . . . . . . . 550
10.8.3 The principle of minimum complementary energy . . . . . . . . . 551
10.8.4 The principle of least work . . . . . . . . . . . . . . . . . . . . . . . . . . . . 553
XVIII Contents
10.8.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 559
10.9 Energy theorems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 560
10.9.1 Clapeyron’s theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 561
10.9.2 Castigliano’s first theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 563
10.9.3 Crotti-Engesser theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 564
10.9.4 Castigliano’s second theorem . . . . . . . . . . . . . . . . . . . . . . . . . . 565
10.9.5 Applications of energy theorems . . . . . . . . . . . . . . . . . . . . . . . 565
10.9.6 The dummy load method . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 570
10.9.7 Unit load method revisited . . . . . . . . . . . . . . . . . . . . . . . . . . . . 572
10.9.8 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 576
10.10Reciprocity theorems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 577
10.10.1Betti’s theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 577
10.10.2Maxwell’s theorem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 579
10.10.3Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 581
11 Variational and approximate solutions . . . . . . . . . . . . . . . . . . . . . . . . . . . . 583
11.1 Approach . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 583
11.2 Rayleigh-Ritz method for beam bending . . . . . . . . . . . . . . . . . . . . . . . 585
11.2.1 Statement of the problem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 585
11.2.2 Description of the Rayleigh-Ritz method . . . . . . . . . . . . . . . . 586
11.2.3 Discussion of the Rayleigh-Ritz method . . . . . . . . . . . . . . . . . 587
11.2.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 602
11.3 The strong and weak statements of equilibrium . . . . . . . . . . . . . . . . . . 603
11.3.1 The weak form for beams under axial loads . . . . . . . . . . . . . . 604
11.3.2 Approximate solutions for beams under axial loads . . . . . . . . 608
11.3.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 616
11.3.4 The weak form for beams under transverse loads . . . . . . . . . . 617
11.3.5 Approximate solutions for beams under transverse loads . . . 621
11.3.6 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 624
11.3.7 Equivalence with energy principles . . . . . . . . . . . . . . . . . . . . . 625
11.3.8 The principle of minimum total potential energy . . . . . . . . . . 627
11.3.9 Treatment of the boundary conditions . . . . . . . . . . . . . . . . . . . 629
11.3.10Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 638
11.4 Formal procedures for the derivation of approximate solutions . . . . . 638
11.4.1 Basic approximations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 639
11.4.2 Principle of virtual work . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 640
11.4.3 The principle of minimum total potential energy . . . . . . . . . . 643
11.4.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 650
11.5 A finite element formulation for beams . . . . . . . . . . . . . . . . . . . . . . . . 654
11.5.1 General description of the problem . . . . . . . . . . . . . . . . . . . . . 655
11.5.2 Kinematics of an element . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 657
11.5.3 Element displacement field . . . . . . . . . . . . . . . . . . . . . . . . . . . . 658
11.5.4 Element curvature field . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 660
11.5.5 Element strain energy and stiffness matrix . . . . . . . . . . . . . . . 660
11.5.6 Element external potential and load array . . . . . . . . . . . . . . . . 661
Contents XIX
11.5.7 Assembly procedure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 662
11.5.8 Alternative description of the assembly procedure . . . . . . . . . 664
11.5.9 Derivation of the governing equations . . . . . . . . . . . . . . . . . . . 666
11.5.10Solution procedure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 666
11.5.11Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 670
11.5.12Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 671
12 Variational and energy principles . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 673
12.1 Mathematical preliminaries . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 673
12.1.1 Stationary point of a function . . . . . . . . . . . . . . . . . . . . . . . . . . 674
12.1.2 Lagrange multiplier method . . . . . . . . . . . . . . . . . . . . . . . . . . . 675
12.1.3 Stationary point of a definite integral . . . . . . . . . . . . . . . . . . . . 677
12.2 Variational and energy principles . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 679
12.2.1 Review of the equations of linear elasticity . . . . . . . . . . . . . . . 680
12.2.2 The principle of virtual work . . . . . . . . . . . . . . . . . . . . . . . . . . 682
12.2.3 The principle of complementary virtual work . . . . . . . . . . . . . 683
12.2.4 Strain and complementary strain energy density functions . . 685
12.2.5 The principle of minimum total potential energy . . . . . . . . . . 686
12.2.6 The principle of minimum complementary energy . . . . . . . . . 688
12.2.7 Energy theorems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 690
12.2.8 Hu-Washizu’s principle . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 690
12.2.9 Hellinger-Reissner’s principle . . . . . . . . . . . . . . . . . . . . . . . . . . 694
12.3 Applications of variational and energy principles . . . . . . . . . . . . . . . . 695
12.3.1 The shear lag problem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 697
12.3.2 The Saint-Venant torsion problem . . . . . . . . . . . . . . . . . . . . . . 701
12.3.3 The Saint-Venant torsion problem using the Prandtl stress
function . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 703
12.3.4 The non-uniform torsion problem. . . . . . . . . . . . . . . . . . . . . . . 707
12.3.5 The non-uniform torsion problem (closed sections) . . . . . . . . 709
12.3.6 The non-uniform torsion problem (open sections) . . . . . . . . . 712
12.3.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 713
Part IV Advanced topics
13 Introduction to plasticity and thermal stresses . . . . . . . . . . . . . . . . . . . . . 721
13.1 Yielding under combined loading . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 721
13.1.1 Introduction to yield criteria . . . . . . . . . . . . . . . . . . . . . . . . . . . 722
13.1.2 Tresca’s criterion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 724
13.1.3 Von Mises’ criterion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 724
13.1.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 725
13.2 Applications of yield criteria to structural problems . . . . . . . . . . . . . . 725
13.2.1 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 731
13.2.2 Plastic bending . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 732
13.2.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 737
XX Contents
13.2.4 Plastic torsion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 737
13.3 Thermal stresses in structures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 741
13.3.1 The direct method . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 742
13.3.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 746
13.3.3 The constraint method . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 746
13.4 Application to bars, trusses and beams . . . . . . . . . . . . . . . . . . . . . . . . . 748
13.4.1 Applications to bars and trusses . . . . . . . . . . . . . . . . . . . . . . . . 748
13.4.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 753
13.4.3 Application to beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 753
13.4.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 760
14 Buckling of beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 763
14.1 Rigid bar with root torsional spring . . . . . . . . . . . . . . . . . . . . . . . . . . . . 763
14.1.1 Analysis of a perfect system . . . . . . . . . . . . . . . . . . . . . . . . . . . 763
14.1.2 Analysis of an imperfect system . . . . . . . . . . . . . . . . . . . . . . . . 765
14.2 Buckling of beams. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 767
14.2.1 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 767
14.2.2 Buckling of a simply-supported beam (equilibrium approach) 769
14.2.3 Buckling of a simply-supported beam (imperfection
approach) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 771
14.2.4 Work done by the axial force . . . . . . . . . . . . . . . . . . . . . . . . . . 774
14.2.5 Buckling of a simply-supported beam (energy approach) . . . 776
14.2.6 Applications to beam buckling . . . . . . . . . . . . . . . . . . . . . . . . . 780
14.2.7 Buckling of beams with various end conditions . . . . . . . . . . . 784
14.2.8 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 784
14.3 Buckling of sandwich beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 789
15 Shearing deformations in beams . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 793
15.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 793
15.1.1 A simplified approach . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 794
15.1.2 An equilibrium approach . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 795
15.1.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 801
15.2 Shear deformable beams: an energy approach . . . . . . . . . . . . . . . . . . . 801
15.2.1 Shearing effects on beam deflections . . . . . . . . . . . . . . . . . . . . 805
15.2.2 Shearing effects on buckling . . . . . . . . . . . . . . . . . . . . . . . . . . . 812
15.2.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 814
16 Kirchhoff plate theory . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 819
16.1 Governing equations of Kirchhoff plate theory . . . . . . . . . . . . . . . . . . 820
16.1.1 Kirchhoff assumptions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 820
16.1.2 Stress resultants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 824
16.1.3 Equilibrium equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 826
16.1.4 Constitutive laws . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 828
16.1.5 Stresses due to in-plane forces and bending moments . . . . . . 830
16.1.6 Summary of Kirchhoff plate theory . . . . . . . . . . . . . . . . . . . . . 830
Contents XXI
16.2 The bending problem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 831
16.2.1 Typical boundary conditions . . . . . . . . . . . . . . . . . . . . . . . . . . . 832
16.2.2 Simple plate bending solutions . . . . . . . . . . . . . . . . . . . . . . . . . 836
16.2.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 839
16.3 Anisotropic plates . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 840
16.3.1 Laminated composite plates . . . . . . . . . . . . . . . . . . . . . . . . . . . 840
16.3.2 Constitutive laws for laminated composite plates . . . . . . . . . . 841
16.3.3 The in-plane stiffness matrix . . . . . . . . . . . . . . . . . . . . . . . . . . . 842
16.3.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 844
16.3.5 The bending stiffness matrix . . . . . . . . . . . . . . . . . . . . . . . . . . . 845
16.3.6 The coupling stiffness matrix . . . . . . . . . . . . . . . . . . . . . . . . . . 847
16.3.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 849
16.3.8 Directionally stiffened plates . . . . . . . . . . . . . . . . . . . . . . . . . . . 849
16.3.9 Governing equations for anisotropic plates . . . . . . . . . . . . . . . 851
16.4 Solution techniques for rectangular plates . . . . . . . . . . . . . . . . . . . . . . 853
16.4.1 Navier’s solution for simply supported plates . . . . . . . . . . . . . 853
16.4.2 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 858
16.4.3 Le´vy’s solution . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 859
16.4.4 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 864
16.5 Circular plates . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 865
16.5.1 Governing equations for the bending of circular plates . . . . . 865
16.5.2 Circular plates subjected to loading presenting circular
symmetry . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 868
16.5.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 871
16.5.4 Circular plates subjected to arbitrary loading . . . . . . . . . . . . . 872
16.5.5 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 874
16.6 Energy formulation of Kirchhoff plate theory . . . . . . . . . . . . . . . . . . . 875
16.6.1 The virtual work done by the internal stresses . . . . . . . . . . . . 876
16.6.2 The virtual work done by the applied loads . . . . . . . . . . . . . . . 880
16.6.3 The principle of virtual work for Kirchhoff plates . . . . . . . . . 881
16.6.4 The principle of minimum total potential energy for
Kirchhoff plates . . .
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 882
16.6.5 Approximate solutions for Kirchhoff plates . . . . . . . . . . . . . . 884
16.6.6 Solutions based on partial approximation . . . . . . . . . . . . . . . . 891
16.6.7 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 895
16.7 Buckling of plates . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 896
16.7.1 Equilibrium formulation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 897
16.7.2 Energy formulation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 904
16.7.3 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 913
A Appendix: mathematical tools . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 915
A.1 Notation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 915
A.2 Vectors, arrays, matrices and linear algebra . . . . . . . . . . . . . . . . . . . . . 916
A.2.1 Vectors, arrays and matrices . . . . . . . . . . . . . . . . . . . . . . . . . . . 916
A.2.2 Vector, array and matrix operations . . . . . . . . . . . . . . . . . . . . . 918
XXII Contents
A.2.3 Solutions of simultaneous linear algebraic equations . . . . . . . 921
A.2.4 Eigenvalues and eigenvectors . . . . . . . . . . . . . . . . . . . . . . . . . . 922
A.2.5 Positive-definite and quadratic forms . . . . . . . . . . . . . . . . . . . . 923
A.2.6 Partial derivatives of a linear form . . . . . . . . . . . . . . . . . . . . . . 924
A.2.7 Partial derivatives of a quadratic form . . . . . . . . . . . . . . . . . . . 924
A.2.8 Stationarity and quadratic forms . . . . . . . . . . . . . . . . . . . . . . . . 925
A.2.9 Minimization and quadratic forms . . . . . . . . . . . . . . . . . . . . . . 925
A.2.10 Least-square solution of linear systems with redundant
equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 926
A.2.11 Problems . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 926
A.3 Coordinate systems and transformations . . . . . . . . . . . . . . . . . . . . . . . 927
A.3.1 The rotation matrix . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 927
A.3.2 Rotation of vector components . . . . . . . . . . . . . . . . . . . . . . . . . 928
A.3.3 The rotation matrix in two dimensions . . . . . . . . . . . . . . . . . . . 929
A.3.4 Rotation of vector components in two dimensions . . . . . . . . . 930
A.4 Orthogonality properties of trigonometric functions . . . . . . . . . . . . . . 930
A.5 Gauss-Legendre quadrature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 931
References . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 935
Index . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 937
1
Basic equations of linear elasticity
Structural analysis is concerned with the evaluation of deformations and stresses aris-
ing within a solid object under the action of applied loads. If time is not explicitly
considered as an independent variable, the analysis is said to be static; otherwise it
is referred to as structural dynamic analysis, or simply structural dynamics. Under
the assumption of small deformations and linearly elastic material behavior, three-
dimensional formulations result in a set of fifteen linear first order partial differential
equations involving the displacement field (three components), the stress field (six
components) and the strain field (six components). This chapter presents the deriva-
tion of these governing equations. In many applications, this complex problem can
be reduced to simpler, two-dimensional formulations called plane stress and plane
strain problems.
For most situations, it is not possible to develop analytical solutions of these
equations. Consequently, structural analysis is concerned with the analysis of struc-
tural components, such as bars, beams, plates, or shells, which will be addressed
in subsequent chapters. In each case, assumptions are made about the behavior of
these structural components, which considerably simplify the analysis process. For
instance, given a suitable set of assumptions, the analysis of bar and beam problems
reduces to the solution of one-dimensional equations for which analytical solutions
are easily obtained.
1.1 The concept of stress
1.1.1 The state of stress at a point
The state of stress in a solid body is a measure of the intensity of forces acting within
the solid. It can be visualized by cutting the solid by a plane normal to unit vector,
n¯, to create two free bodies which reveal the forces acting on the exposed surfaces.
From basic statics, it is well-known that the distribution of forces and moments that
will appear on the surface of the cut can be represented by an equipollent force, F ,
acting at a point of the surface and a couple, M . Newton’s 3rd law also requires
4 1 Basic equations of linear elasticity
a force and couple of equal magnitudes and opposite directions to act on the two
surfaces created by the cut through the solid, as depicted in fig. 1.1. (See appendix A
for a description of the vector, array and matrix notations used in this text.)
M
M
Mn M
A
n
SolidBody
FreeBody
diagram
Smallsurface
onthecut
F
Fn
F
F
Planeof
thecut
P
n
n
Appliedloads
Fig. 1.1. A solid body cut by a plane to isolate a free body.
Consider now a small surface of area An located at point P on the surface gen-
erated by the cut in the solid. The forces and moments acting on this surface are
equipollent to a force, Fn, and couple, Mn; note that these resultants are, in gen-
eral, different, in both magnitude and orientation, from the corresponding resultants
acting on the entire surface of the cut, as shown in fig. 1.1. Let the small surface be
smaller and smaller until it becomes an element of infinitesimal area dAn → 0. As
the surface shrinks to a differential size, the force and couple acting on the element
keep decreasing in magnitude and changing in orientation whereas the normal to the
surface remains the unit vector n¯ of constant direction in space. This limiting process
gives rise to the concept of stress vector, which is defined as
τn = lim
dAn→0
(
Fn
dAn
)
. (1.1)
The existence of the stress vector, i.e., the existence of the limit in eq. (1.1), is
a fundamental assumption of continuum mechanics. In this limiting process, it is as-
sumed that the couple, Mn, becomes smaller and smaller and, in the limit, Mn → 0
as dAn → 0; this is also an assumption of continuum mechanics which seems to
be reasonable because in the limiting process, both forces and moment arms become
increasingly small. Forces decrease because the area they act on decreases and mo-
ment arms decrease because the dimensions of the surface decrease. At the limit, the
couple is the product of a differential element of force by a differential element of
moment arm, giving rise to a negligible, second order differential quantity.
In conclusion, whereas an equipollent couple might act on the entire surface of
the cut, the equipollent couple is assumed to vanish on a differential element of area
of the same cut. The total force acting on a differential element of area, dAn, is
1.1 The concept of stress 5
Fn = dAn τn. (1.2)
Clearly, the stress vector has units of force per unit area. In the SI system, this is
measured in Newton per square meters, or Pascals (Pa).
During the limiting process de-
i1
i3
i2
t3
t
1
t2
s3
s1
s2
t31 t21
t23
t13
t12
t32
dA3
dA2
dA1
P
P
P
Cutnormal
toaxis i3
Cutnormal
toaxis i2
Cutnormal
toaxis i1
Fig. 1.2. A rigid body cut at point P by three planes
orthogonal to the Cartesian axes.
scribed in the previous paragraph,
the surface orientation, as defined
by the normal to the surface, is kept
constant in space. Had a different
normal been selected, a different
stress vector would have been ob-
tained.
To illustrate this point, con-
sider a solid body and a coordinate
system, I, consisting of three mu-
tually orthogonal unit vectors, I =
(¯ı1, ı¯2, ı¯3), as shown in fig. 1.2.
First, the solid is cut at point P by a
plane normal to axis ı¯1; on the sur-
face of the cut, at point P, a differ-
ential element of surface with an
area dA1 is defined and let τ1 be
the stress vector acting on this face. Next, the solid is cut at the same point by a
plane normal to axis ı¯2; at point P, let τ2 be the stress vector acting on the differ-
ential element of surface with an area dA2. Finally, the process is repeated a third
time for a plane normal to axis ı¯3; at point P, the stress vector τ3 is acting on the
differential element of surface with an area dA3. Clearly, three stress vectors, τ1, τ2,
and τ3 are acting at the same point P, but on three mutually orthogonal faces normal
to axes ı¯1, ı¯2, and ı¯3, respectively. Because these three stress vectors are acting on
three faces with different orientations, there is no reason to believe that those stress
vectors should be identical.
To further understand the state of stress at point P, the components of each stress
vectors acting on the three faces are defined
τ1 = σ1 ı¯1 + τ12 ı¯2 + τ13 ı¯3, (1.3a)
τ2 = τ21 ı¯1 + σ2 ı¯2 + τ23 ı¯3, (1.3b)
τ3 = τ31 ı¯1 + τ32 ı¯2 + σ3 ı¯3. (1.3c)
The stress components σ1, σ2, and σ3 are called direct, or normal stresses; they
act on faces normal to axes ı¯1, ı¯2, and ı¯3, respectively, in directions along axes ı¯1,
ı¯2, and ı¯3, respectively. The stress components τ12 and τ13 are called shearing or
shear stresses; both act on the face normal to axis ı¯1, in directions of axes ı¯2 and ı¯3,
respectively. Similarly, stress components τ21 and τ23 both act on the face normal to
axis ı¯2, in directions of axes ı¯1 and ı¯3, respectively. Finally, stress components τ31
and τ32 both act on the face normal to axis ı¯3, in directions along axes ı¯1 and ı¯2,
6 1 Basic equations of linear elasticity
respectively. The various stress components appearing in eq. (1.3) are referred to as
the engineering stress components. The units of stress components are identical to
those of the stress vector, force per unit area, or Pascal.
The stress components represented
s
1
s
1
s
2
s
2
s
3
s
3
t
12
t
12
t
13
t
13
t
23
t
23
t
21
t
21
t
31
t
31
t
32
t
32
i1
i2
i3
Fig. 1.3. Sign conventions for the stress com-
ponents acting on a differential volume ele-
ment. All stress components shown here are
positive.
in fig. 1.2 are all defined as positive.
Furthermore, the three faces depicted
in this figure are positive faces. A face
is positive when the outward normal to
the face, i.e., the normal pointing away
from the body, is in the same direction
as the axis to which the face is normal;
a face is negative when its outward nor-
mal is pointing in the direction opposite
to the axis to which the face is normal.
The positive directions of stress com-
ponents acting on negative faces are the
opposite of those for stress components
acting on positive faces. This sign con-
vention is illustrated in fig. 1.3, which
shows positive stress components acting on the six faces of a cube of differential
size. Positive stress components are shown in solid lines on the three positive faces
of the cube; positive stress components are shown in dotted lines on the three nega-
tive (hidden) faces of the cube.
Taken together, the direct stress components σ1, σ2, and σ3 and the shear stress
components, τ12 and τ13, τ21 and τ23, and τ31 and τ32, fully characterize the state
of stress at point P. It will be shown in a later section that if the stress components
acting on three orthogonal faces are known, it is possible to compute the stress com-
ponents acting at the same point, on a face of arbitrary orientation. This discussion
underlines the fact that the state of stress at a point is a complex concept: its complete
definition requires the knowledge of nine stress components acting on three mutually
orthogonal faces.
This should be contrasted with the concept of force. A force is vector quantity
that is characterized by its magnitude and orientation. Alternatively, a force can be
defined by the three components of the force vector in a given coordinate system.
The definition of a force thus requires three quantities, whereas the definition of the
stress state requires nine quantities.
A force is a vector, which is referred to as a first order tensor, whereas a state of
stress is a second order tensor. Several quantities commonly used in solid mechanics
are also second order tensors: the strain tensor, the bending stiffnesses of a beam,
and the mass moments of inertia of a solid object. The first two of these quantities
will be introduced in later sections and chapters. Much like the case for vectors, all
second order tensors will be shown to possess certain common characteristics.
1.1 The concept of stress 7
1.1.2 Volume equilibrium equations
In general, the state of stress varies throughout a solid body, and hence, stresses
acting on two parallel faces located a small distance apart are not equal. Consider,
for instance, the two opposite faces of a differential volume element that are normal
to axis ı¯2, as shown in fig. 1.4. The axial stress component on the negative face at
coordinate x2 is σ2, but the stress components on the positive face at coordinate
x2 + dx2 will be slightly different and written as σ2(x2 + dx2). If σ2(x2) is an
analytic function, it is then possible to express σ2(x2 + dx2) in terms of σ2(x2)
using a Taylor series expansion to find
σ2(x2 + dx2) = σ2(x2) +
∂σ2
∂x2
∣∣∣∣
x2
dx2 + . . .higher order terms in dx2.
This expansion is a fundamental step in the derivation of the differential equa-
tions governing the behavior of a continuum. The stress component on the positive
face at coordinate x2+dx2 can be written as σ2(x2+dx2) ≈ σ2+ (∂σ2/∂x2)dx2.
The same Taylor series expansion technique can be applied to all other direct and
shear stress components.
i1
i2
i3
s s3 3 3 3+(d /dx)dx
s3
s s2 2 2 2+(d /dx)dx
t t32 32 3 3+(d /dx)dx
t32
t t31 31 3 3+(d /dx)dx
t31
t t23 23 2 2+(d /dx)dx
t23 t t21 21 2 2+(d /dx)dx
t21
s
2
Fig. 1.4. Stress components acting on a differential element of volume. For clarity of the
figure, the stress components acting on the faces normal to ı¯1 are not shown.
Consider now the differential element of volume depicted in fig. 1.4. It is sub-
jected to stress components acting on its six external faces and to body forces per
unit volume, represented by a vector b acting at its centroid. These body forces could
be gravity forces, inertial forces, or forces of an electric or magnetic origin; the com-
ponents of this body force vector resolved in coordinate system I = (¯ı1, ı¯2, ı¯3) as
b = b1 ı¯1 + b2 ı¯2 + b3 ı¯3. The units of the force vector are force per unit volume or
Newton per cubic meter.
Force equilibrium
According to Newton’s law, static equilibrium requires the sum of all the forces
acting on this differential element to vanish. Considering all the forces acting along
8 1 Basic equations of linear elasticity
the direction of axis ı¯1, the equilibrium condition is
− σ1 dx2dx3 +
(
σ1 +
∂σ1
∂x1
dx1
)
dx2dx3
− τ21 dx1dx3 +
(
τ21 +
∂τ21
∂x2
dx2
)
dx1dx3
− τ31 dx1dx2 +
(
τ31 +
∂τ31
∂x3
dx3
)
dx1dx2
+ b1 dx1dx2dx3 = 0.
This equation states an equilibrium of forces, and therefore the stress components
must be multiplied by the area of the surface on which they act to yield the corre-
sponding force. Similarly, the component of the body force per unit volume of the
body is multiplied by the volume of the differential element, dx1dx2dx3, to give
the body force acting on the element. After simplification, this equilibrium condition
becomes [
∂σ1
∂x1
+
∂τ21
∂x2
+
∂τ31
∂x3
+ b1
]
dx1dx2dx3 = 0.
This equation is satisfied when the expression in brackets vanishes, and this
yields the equilibrium equation in the direction of axis ı¯1
∂σ1
∂x1
+
∂τ21
∂x2
+
∂τ31
∂x3
+ b1 = 0.
For the same reasons, forces along axes ı¯2 and ı¯3 must vanish as well, and a similar
reasoning yields the following three equilibrium equations
∂σ1
∂x1
+
∂τ21
∂x2
+
∂τ31
∂x3
+ b1 = 0, (1.4a)
∂τ12
∂x1
+
∂σ2
∂x2
+
∂τ32
∂x3
+ b2 = 0, (1.4b)
∂τ13
∂x1
+
∂τ23
∂x2
+
∂σ3
∂x3
+ b3 = 0, (1.4c)
which must be satisfied at all points inside the body.
The equilibrium conditions implied by Newton’s law, eqs. (1.4), have been writ-
ten by considering an differential element of the undeformed body. Of course, when
forces are applied, the body deforms and so does every single differential element.
Strictly speaking, equilibrium should be enforced on the deformed configuration of
the body, rather than its undeformed configuration. Indeed, stresses are only present
when external forces are applied and the body is deformed. When no forces are ap-
plied, the body is undeformed, but stresses all vanish.
Unfortunately, it is difficult to write equilibrium conditions on the deformed con-
figuration of the body because this configuration is unknown; indeed, the goal of
the theory of elasticity is to predict the deformation of elastic bodies under load.
It is a basic assumption of the linear theory of elasticity developed here that the
displacements of the body under the applied loads are very small, and hence, the
1.1 The concept of stress 9
difference between the deformed and undeformed configurations of the body is very
small. Under this assumption, it is justified to impose equilibrium conditions to the
undeformed configuration of the body, because it is nearly identical to its deformed
configuration.
Moment equilibrium
To satisfy all equilibrium requirements, the sum of all the moments acting on the
differential element of volume depicted in fig. 1.4 must also vanish. Consider first
the moment equilibrium about axis ı¯1. The contributions of the direct stresses and of
the body forces can be eliminated by choosing an axis passing through the center of
the differential element. The resulting moment equilibrium equation is
τ23 dx1dx3
dx2
2
+
(
τ23 +
∂τ23
∂x2
dx2
)
dx1dx3
dx2
2
−τ32 dx1dx2 dx32 −
(
τ32 +
∂τ32
∂x3
dx3
)
dx1dx2
dx3
2
=
[
τ23 − τ32 + ∂τ23
∂x2
dx2
2
− ∂τ32
∂x3
dx3
2
]
dx1dx2dx3 = 0.
The bracketed expression must vanish and after neglecting higher order terms, this
reduces to the following equilibrium condition
τ23 − τ32 = 0.
Enforcing the vanishing of the sum of
t
t
t
t
90
o
90
o
Fig. 1.5. Reciprocity of the shearing
stresses acting on two orthogonal faces.
the moments about axes ı¯2 and ı¯3 leads to
similar equations,
τ23 = τ32, τ13 = τ31, τ12 = τ21. (1.5)
The implication of these equalities is sum-
marized by the principle of reciprocity
of shear stresses, which is illustrated in
fig. 1.5.
Principle 1 (Principle of reciprocity of shear stresses) Shear stresses acting in
the direction normal to the common edge of two orthogonal faces must be equal in
magnitude and be simultaneously oriented toward or away from the common edge.
Another implication of the reciprocity of the shear stresses is that of the nine
components of stresses, six only are independent. It is common practice to arrange
the stress tensor components in a 3×3 matrix format σ1 τ12 τ13τ12 σ2 τ23
τ13 τ23 σ3
 . (1.6)
The principle of reciprocity implies the symmetry of the stress tensor.
10 1 Basic equations of linear elasticity
1.1.3 Surface equilibrium equations
At the outer surface of the body, the stresses acting inside the body must be in equi-
librium with the externally applied surface tractions. Surface tractions are repre-
sented by a stress vector, t, that can be resolved in reference frame I = (¯ı1, ı¯2, ı¯3) as
t = t1 ı¯1+t2 ı¯2+t3 ı¯3. Figure 1.6 shows a free body in the form of a differential tetra-
hedron bounded by three negative faces cut through the body in directions normal to
axes ı¯1, ı¯2, and ı¯3, and by a fourth face, ABC, of area dAn, which is a differential
element of the outer surface of the body. The unit normal to this element of area is
denoted n¯, and its components in coordinate system I are n¯ = n1 ı¯1+n2 ı¯2+n3 ı¯3.
Note that n1, n2, and n3 are the cosines of the angle between n¯ and ı¯1, n¯ and ı¯2, and
n¯ and ı¯3, respectively, also called the direction cosines of n¯: n1 = n¯ · ı¯1 = cos(n¯, ı¯1),
n2 = n¯ · ı¯2 = cos(n¯, ı¯2), and n3 = n¯ · ı¯3 = cos(n¯, ı¯3).
Fig. 1.6. A tetrahedron with one face along the outer surface of the body.
Equilibrium of forces acting along axis ı¯1 implies
t1dAn = σ1dA1 + τ21dA2 + τ31dA3 − b1 dx1dx2dx36 , (1.7)
where dA1, dA2, and dA3 are the areas of triangles OBC, OAC and OAB, respec-
tively, and the last term represents the body force times the volume of the tetrahe-
dron. The areas of the three faces normal to the axes are found by projecting face
ABC onto planes normal to the axes using the direction cosines to find
dA1 = n1dAn, dA2 = n2dAn, and dA3 = n3dAn. (1.8)
Dividing eq. (1.7) by dAn then yields the first component of the surface traction
vector
t1 = σ1n1 + τ21n2 + τ31n3,
where the body force term vanishes because it is a higher order differential term.
The same procedure can be followed to express equilibrium conditions along the
1.2 Analysis of the state of stress at a point 11
directions of axes ı¯2 and ı¯3. The three components of the surface traction vector then
become
t1 = σ1 n1 + τ12 n2 + τ13 n3, (1.9a)
t2 = τ12 n1 + σ2 n2 + τ23 n3, (1.9b)
t3 = τ31 n1 + τ32 n2 + σ3 n3. (1.9c)
A body is said to be in equilibrium if eqs. (1.4) are satisfied at all points inside
the body, and eqs. (1.9) are satisfied at all points of its external surface.
1.2 Analysis of the state of stress at a point
The state of stress at a point is characterized in the previous section by the normal
and shear stress components acting on the faces of a differential element of volume
cut from the solid. The faces of this cube are cut normal to the axes of a Cartesian ref-
erence frame I = (¯ı1, ı¯2, ı¯3), and the stress vector acting on these faces are resolved
along the same axes. Clearly, another face at an arbitrary orientation with respect to
these axes can be selected. In section 1.2.1, it will be shown that the stresses acting
on this face can be related to the stresses acting on the faces normal to axes ı¯1, ı¯2, and
ı¯3. This important result implies that once the stress components are known on three
mutually orthogonal faces at a point, they are known on any face passing through that
point. Hence, the state of stress at a point is fully defined once the stress components
acting on three mutually orthogonal faces at a point are known.
1.2.1 Stress components acting on an arbitrary face
To establish relationships between stresses, it is necessary to consider force or mo-
ment equilibrium due to these stresses, and this must be done with reference to a
specific free body diagram. Figure 1.7 shows a specific free body constructed from a
tetrahedron defined by three faces cut normal to axes ı¯1, ı¯2, and ı¯3, and a fourth face
normal to unit vector n¯ = n1 ı¯1