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Introductory Finite Element Method 1st Edition Chandrakant S. Desai
Introductory Finite Element Method 1st Edition
Chandrakant S. Desai Digital Instant Download
Author(s): Chandrakant S. Desai, TribikramKundu
ISBN(s): 9780849302435, 0849302439
Edition: 1
File Details: PDF, 4.70 MB
Year: 2001
Language: english
Introductory Finite Element Method 1st Edition Chandrakant S. Desai
FINITEELEMENT
METHOD
Introductory
Published Titles
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Finite Element Method Using MATLAB, 2nd
Edition
Young W. Kwon & Hyochoong Bang
Fundamentals of Environmental Discharge Modeling
Lorin R. Davis
Introductory Finite Element Method
Chandrakant S. Desai & Tribikram Kundu
Intelligent Transportation Systems: New Principles and Architectures
Sumit Ghosh & Tony Lee
Mathematical & Physical Modeling of Materials Processing Operations
Olusegun Johnson Ileghus, Manabu Iguchi & Walter E. Wahnsiedler
Mechanics of Composite Materials
Autar K. Kaw
Mechanics of Fatigue
Vladimir V. Bolotin
Mechanism Design: Enumeration of Kinematic Structures According
to Function
Lung-Wen Tsai
Nonlinear Analysis of Structures
M. Sathyamoorthy
Practical Inverse Analysis in Engineering
David M. Trujillo & Henry R. Busby
Principles of Solid Mechanics
Rowland Richards, Jr.
Thermodynamics for Engineers
Kau-Fui Wong
Viscoelastic Solids
Roderic S. Lakes
Forthcoming Titles
Distributed Generation: The Power Paradigm for the New Millennium
Anne-Marie Borbely & Jan F. Kreider
Engineering Experimentation
Euan Somerscales
Fluid Power Circuits and Control: Fundamentals and Applications
John S. Cundiff
Heat Transfer in Single and Multiphase Systems
Greg F. Naterer
Mechanics of Solids & Shells
Gerald Wempner & Demosthenes Talaslidis
Mechanical Engineering Series
Frank Kreith - Series Editor
Chandrakant S. Desai
Tribikram Kundu
FINITEELEMENT
METHOD
Introductory
Boca Raton London New York Washington, D.C.
CRC Press
This book contains information obtained from authentic and highly regarded sources. Reprinted material
is quoted with permission, and sources are indicated. A wide variety of references are listed. Reasonable
efforts have been made to publish reliable data and information, but the author and the publisher cannot
assume responsibility for the validity of all materials or for the consequences of their use.
Neither this book nor any part may be reproduced or transmitted in any form or by any means, electronic
or mechanical, including photocopying, microfilming, and recording, or by any information storage or
retrieval system, without prior permission in writing from the publisher.
The consent of CRC Press LLC does not extend to copying for general distribution, for promotion, for
creating new works, or for resale. Specific permission must be obtained in writing from CRC Press LLC
for such copying.
Direct all inquiries to CRC Press LLC, 2000 N.W. Corporate Blvd., Boca Raton, Florida 33431.
Trademark Notice: Product or corporate names may be trademarks or registered trademarks, and are
used only for identification and explanation, without intent to infringe.
Visit the CRC Press Web site at www.crcpress.com
© 2001 by CRC Press LLC
No claim to original U.S. Government works
International Standard Book Number 0-8493-0243-9
Library of Congress Card Number 2001017466
Printed in the United States of America 1 2 3 4 5 6 7 8 9 0
Printed on acid-free paper
Library of Congress Cataloging-in-Publication Data
Desai, C. S. (Chandrakant S.), 1936-
Introductory finite element method / Chandrakant S. Desai, Tribikram Kundu.
p. cm.
Includes bibliographical references and index.
ISBN 0-8493-0243-9 (alk. paper)
1. Finite element method. I. Kundu, T. (Tribikram). II. Title.
TA347.F5 .D48 2001
620′.001′1535--dc21 2001017466
0618fm/frame Page 4 Wednesday, April 11, 2001 9:27 AM
Dedication
To
Our wives: Patricia Desai
and Nupur Kundu
Children: Maya and Sanjay; Ina and Auni
and Parents: Sankalchand Desai and Kamala Desai;
Makhan Lal Kundu and Sandhya Rani Kundu
0618fm/frame Page 5 Wednesday, April 11, 2001 9:27 AM
0618fm/frame Page 6 Wednesday, April 11, 2001 9:27 AM
Preface
The finite element method has gained tremendous attention and popularity.
The method is now taught at most universities and colleges, is researched
extensively, and is used by the practicing engineers, industry, and government
agencies. The teaching of the method has been concentrated at the postgrad-
uate level. In view of the growth and wide use of the method, however, it
becomes highly desirable and necessary to teach it at the undergraduate level.
There are a number of books and publications available on the finite ele-
ment method. It appears that almost all of them are suitable for the advanced
students and require a number of prerequisites such as theories of constitu-
tive or stress-strain laws, mechanics, and variational calculus. Some of the
introductory treatments have presented the method as an extension of matrix
methods of structural analysis. This viewpoint may no longer be necessary,
since the finite element method has reached a significant level of maturity
and generality. It has acquired a sound theoretical basis, and in itself has been
established as a general procedure relevant to engineering and mathematical
physics. These developments permit its teaching and use as a general tech-
nique from which applications to topics such as mechanics, structures, geo-
mechanics, hydraulics, and environmental engineering arise as special cases.
It is therefore essential that the method be treated as a general procedure and
taught as such.
This book is intended mainly for the undergraduate and beginning gradu-
ate students. Its approach is sufficiently elementary so that it can be intro-
duced with the background of essentially undergraduate subjects. At the
same time, the treatment is broad enough so that the reader or the teacher
interested in various topics such as stress-deformation analysis, fluid and
heat flow, potential flow, time-dependent problems, diffusion, torsion, and
wave propagation can use and teach from it. The book brings out the intrinsic
nature of the method that permits confluence of various disciplines and pro-
vides a distinct and rather novel approach for teaching the finite element
method at an elementary level. The book can be used for any student with no
prior exposure to the finite element method. The prerequisites for under-
standing the material will be undergraduate mathematics, strength of mate-
rials, and undergraduate courses in structures, hydraulics, geotechnical
engineering, and matrix algebra. Introductory knowledge of computer pro-
gramming is desirable but not necessary. The text is written in such a way
that no prior knowledge of variational principles is necessary. Over a period
of the last 30 years or so, the authors have taught, based on these prerequi-
sites, an undergraduate course and a course for user groups composed of
beginners. This experience has shown that undergraduates or beginners
0618fm/frame Page 7 Wednesday, April 11, 2001 9:27 AM
equipped with these prerequisites, available to them in the undergraduate
curricula at most academic institutions, can understand and use the material
presented in this book.
The first chapter presents a rather philosophical discussion of the finite ele-
ment method and often defines various terms on the basis of eastern and
western concepts from antiquity. The second chapter gives a description of
the eight basic steps and fundamental principles of variational calculus.
Chapters 3 to 5 cover one-dimensional problems in stress-deformation anal-
ysis and steady and time-dependent flow of heat and fluids. The fundamen-
tal generality of the method is illustrated by showing the common
characteristics of the formulation for these topics and by indicating the fact
that their governing equations are essentially similar. The generality is fur-
ther established by including computer codes in Chapter 6 that can solve dif-
ferent types of problems.
Understanding and using the finite element method are closely linked with
the use of the computer. It is the belief of the authors that strictly theoretical
teaching of the method may not give the student an idea of the details and
the ranges of applicability of the technique. Consequently this text endeavors
to introduce the student, gradually and simultaneously with the theoretical
teaching, to the use and understanding of computer codes. The codes pre-
sented in Chapter 6 are thoroughly documented and detailed so that they can
be used and understood without difficulty. Details of these codes, designed
for the beginner, are given in Appendix 3. It is recommended that these or
other available codes be used by the student while learning various topics in
this book.
Chapter 7 introduces the idea of higher-order approximation for the problem
of beam bending and beam-column. One-dimensional problems in mass trans-
port (diffusion-convection) and wave propagation are covered in Chapters 8
and 9, respectively. These problems illustrate, by following the general proce-
dure, formulations for different categories of time-dependent problems.
Chapter 10 presents the basic finite element formulation for two- and three-
dimensional problems. Then in Chapters 11 to 14 different types of two-
dimensional problems are presented. The chapters on Torsion (Chapter 11)
and Other Field Problems (Chapter 12) have been chosen because they
involve only one degree-of-freedom at a point. Chapters 13 and 14 cover two-
dimensional stress-deformation problems involving two and higher degrees-
of-freedom at a point.
The text presents the finite element method by using simple problems. It
must be understood, however, that it is for the sake of easy introduction that
we have used relatively simple problems. The main thrust of the method, on
the other hand, is for solving complex problems that cannot be easily solved
by the conventional procedures.
For a thorough understanding of the finite element method, it is essential
that the students perform hand calculations. With this in mind, most chapters
include a number of problems to be solved by hand calculations. They also
include problems for home assignments and self-study.
0618fm/frame Page 8 Wednesday, April 11, 2001 9:27 AM
The formulations have been presented by using both the variational and
residual procedures. In the former, the potential, complementary, hybrid, and
mixed procedures have been discussed. In the residual procedures, main
attention has been given to Galerkin’s method. A number of other residual
methods are also becoming popular. They are described, therefore, in
Appendix 1, which gives descriptions, solutions, and comparisons for a
problem by using a number of methods: closed-form, Galerkin, collocation,
subdomain, least squares, Ritz, finite difference, and finite element.
Formulations by the finite element method usually result in algebraic
simultaneous equations. Detailed description of these methods is beyond the
scope of this book. Included in Appendix 2, however, are brief introductions
to the commonly used direct and iterative procedures for the solution of alge-
braic simultaneous equations.
Appendix 3 presents details of a number of computer codes relevant to var-
ious topics in the text.
The book can be used for one or two undergraduate courses. The second
course may overlap with or be an introductory graduate course. Although a
number of topics have been covered in the book, a semester or quarter
course could include a selected number of topics. For instance, a quarter
course can cover Chapters 1 to 6, and then one or two topics from the
remaining chapters. For a class interested in mechanics and stress-deforma-
tion analyses, the topics can be Beam Bending and Beam-Column
(Chapter 7), and Two-Dimensional Stress Deformation (Chapters 10 and 13).
If time is available (in the case of a semester course), Chapter 9 on One-
Dimensional Stress Wave Propagation, Chapter 11 on Torsion, and/or
Chapter 14 on Multicomponent Systems can be added. A class oriented
toward field problems and hydraulics can choose one or more of Chapters 8,
9, 11, and 12 in addition to Chapters 1 to 6 and 10.
We would like to express special appreciation to Jose Franscisco Perez Avila
for his assistance in the manuscript preparation and Shashank Pradhan for
implementing some of the computer codes and preparation of user’s manuals.
We realize that it is not easy to write at an elementary level for the finite ele-
ment method with so many auxiliary disciplines. The judgment of this book
is better left to the readers.
Many natural systems can be considered continuous or interconnected,
and their behavior is influenced by a large number of parameters. In order to
understand such a system, we must understand all the parameters. Since this
is not possible we make approximations, by selecting only the significant of
them and neglecting the others. Such a procedure allows understanding of
the entire system by comprehending its components taken one at a time.
These approximations or models obviously involve errors, and we strive con-
tinuously to improve the models and reduce the errors.
Chandrakant S. Desai
Tribikram Kundu
Tucson, Arizona
0618fm/frame Page 9 Wednesday, April 11, 2001 9:27 AM
0618fm/frame Page 6 Wednesday, April 11, 2001 9:27 AM
Authors
Chandrakant S. Desai is a Regents’ Profes-
sor and Director of the Material Modeling
and Computational Mechanics Center,
Department of Civil Engineering and Engi-
neering Mechanics, University of Arizona,
Tucson. He was a Professor in the Depart-
ment of Civil Engineering, Virginia Poly-
technic Institute and State University,
Blacksburg, from 1974 to 1981, and a
Research Civil Engineer at the U.S. Army
Engineer Waterways Experiment Station,
Vicksburg, MS from 1968 to 1974.
Dr. Desai has made original and signifi-
cant contributions in basic and applied
research in material modeling and testing,
and computational methods for a wide
range of problems in civil engineering,
mechanics, mechanical engineering, and
electronic packaging. He has authored/edited 20 books and 18 book chap-
ters, and has been the author/coauthor of over 270 technical papers. He was
the founder and General Editor of the International Journal for Numerical and
Analytical Methods in Geomechanics from 1977 to 2000, and he has served as a
member of the editorial boards of 12 journals.
Dr. Desai has also been a chair/member of a number of committees of var-
ious national and international societies. He is the President of the Interna-
tional Association for Computer Methods and Advances in Geomechanics.
Dr. Desai has also received a number of recognitions: Meritorious Civilian
Service Award by the U.S. Corps of Engineers, Alexander von Humboldt Stif-
tung Prize by the German Government, Outstanding Contributions Medal in
Mechanics by the International Association for Computer Methods and
Advances in Geomechanics, Distinguished Contributions Medal by the
Czech Academy of Sciences, Clock Award by ASME (Electrical and Electronic
Packaging Division), Five Star Faculty Teaching Finalist Award, and the
El Paso Natural Gas Foundation Faculty Achievement Award at the Univer-
sity of Arizona, Tucson.
0618fm/frame Page 11 Wednesday, April 11, 2001 9:27 AM
Professor T. Kundu received his bachelor
degree in mechanical engineering from the
Indian Institute of Technology, Kharagpur
in 1979. His M.S. and Ph.D. were in the field
of mechanics from the Mechanical and
Aerospace Engineering Department of the
University of California, Los Angeles in
1980 and 1983, respectively. He joined the
University of Arizona as an assistant pro-
fessor in 1983 and was promoted to full
professor in 1994.
Dr. Kundu has made significant and orig-
inal contributions in both basic and applied
research in computational mechanics and
nondestructive evaluation (NDE) of mate-
rials by ultrasonic and acoustic microscopy
techniques. He is editor or coeditor of 8 books, coauthor of a textbook, author
of a book chapter, and author/coauthor of over 130 technical papers; half of
those have been published in refereed journals. He is a Fellow of ASME
(American Society of Mechanical Engineers) and ASCE (American Society of
Civil Engineers). He has received a number of awards, including the Presi-
dent’s Gold Medal from IIT, the UCLA Alumni Award, the Humboldt Fel-
lowship from Germany, and the Best Paper Award from the International
Society for Optical Engineering (SPIE). He has extensive research collabora-
tions with international and U.S. scientists. He has spent 21 months as an
Alexander von Humboldt Scholar in the Department of Biology, J. W. Goethe
University, Frankfurt, Germany. He has also spent several months as a visit-
ing professor at a number of other institutes — Department of Mechanics,
Chalmers University of Technology, Gothenberg, Sweden; Acoustic Micros-
copy Center, Semienov Institute of Chemical Physics, Russian Academy of
Science, Moscow; Department of Civil Engineering, EPFL (Swiss Federal
Institute of Technology in Lausanne), Switzerland; Department of Mechani-
cal Engineering, University of Technology of Compiegne, France; Materials
Laboratory, University of Bordeaux, France; LESiR Laboratory, Ecole Nor-
male Superior (ENS), Cachan, France; Aarhus University Medical School,
Aarhus, Denmark; Wright-Patterson Material Laboratory, Dayton, OH.
0618fm/frame Page 12 Wednesday, April 11, 2001 9:27 AM
Contents
1 Introduction ..................................................................................... 1
Basic Concept...........................................................................................................1
Process of Discretization ........................................................................................3
Subdivision .....................................................................................................3
Continuity .......................................................................................................4
Convergence ...................................................................................................4
Bounds.............................................................................................................5
Error .................................................................................................................6
Principles and Laws................................................................................................7
Cause and Effect....................................................................................................10
Important Comment....................................................................................10
Review Assignments ............................................................................................10
Home Assignment 1 .................................................................................... 11
Home Assignment 2 ....................................................................................12
References ............................................................................................... 12
2 Steps in the Finite Element Method ............................................ 13
Introduction ...........................................................................................................13
General Idea...........................................................................................................13
Step 1. Discretize and Select Element Configuration.................14
Step 2. Select Approximation Models or Functions...................16
Step 3. Define Strain (Gradient)-Displacement (Unknown)
and Stress–Strain (Constitutive) Relationships .............18
Step 4. Derive Element Equations ................................................19
Energy Methods ...........................................................................................19
Stationary Value ...........................................................................................20
Potential Energy...........................................................................................20
Method of Weighted Residuals..................................................................22
Element Equations .......................................................................................25
Step 5. Assemble Element Equations to Obtain Global or
Assemblage Equations and Introduce Boundary
Conditions ..........................................................................26
Boundary Conditions ..................................................................................27
Step 6. Solve for the Primary Unknowns ....................................29
Step 7. Solve for Derived or Secondary Quantities....................29
Step 8. Interpretation of Results....................................................29
Introduction to Variational Calculus..................................................................30
Definitions of Functions and Functionals.................................................30
Variations of Functions................................................................................31
Stationary Values of Functions and Functionals .........................36
0618fm/frame Page 13 Wednesday, April 11, 2001 9:27 AM
∆fx to ∆f Conversion .....................................................................................37
More on the Stationary Value of a Functional — Physical
Interpretation....................................................................................38
Natural and Forced Boundary Conditions...............................................39
Two-Dimensional Problems .......................................................................41
Summary ................................................................................................................47
Problems.................................................................................................................48
References ............................................................................................... 50
3 One-Dimensional Stress Deformation ........................................ 53
Introduction ...........................................................................................................53
Step 1. Discretization and Choice of Element
Configuration .....................................................................53
Explanation of Global and Local Coordinates..................................................54
Local and Global Coordinate System for the One-Dimensional Problem .....55
Step 2. Select Approximation Model or Function
for the Unknown (Displacement)....................................56
Generalized Coordinates ............................................................................57
Interpolation Functions........................................................................................60
Relation between Local and Global Coordinates .............................................61
Variation of Element Properties.................................................................61
Requirements for Approximation Functions ....................................................62
Step 3. Define Strain-Displacement and Stress–Strain
Relations..............................................................................64
Stress–Strain Relation...........................................................................................65
Step 4. Derive Element Equations ................................................66
Principle of Minimum Potential Energy............................................................66
Functional for One-Dimensional Stress Deformation Problem ............69
Total Potential Energy Approach...................................................69
Variational Principle Approach......................................................71
Expansion of Terms...............................................................................................73
Integration..............................................................................................................75
Comment.......................................................................................................77
Step 5. Assemble Element Equations to Obtain Global
Equations ............................................................................77
Direct Stiffness Method........................................................................................80
Boundary Conditions ...........................................................................................82
Types of Boundary Conditions ..................................................................83
Homogeneous or Zero-Valued Boundary Condition .............................83
Nonzero Boundary Conditions..................................................................84
Step 6. Solve for Primary Unknowns: Nodal
Displacements ....................................................................85
Step 7. Solve for Secondary Unknowns; Strains and
Stresses ................................................................................88
Strains and Stresses...............................................................................................88
Step 8. Interpretation and Display of Results .............................90
0618fm/frame Page 14 Wednesday, April 11, 2001 9:27 AM
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[45] V. Löfgrenin suomentamina.
[46] Jos tahtoo verrata, mimmoinen taiteellisten tarkoitusten
ohjaama teatterinjohto on käsityöntapaiseen verrattuna,
asetettakoon rinnakkain Åhmanin teatteriseuran repertoari täällä
vuonna 1866-67 ja nykyinen. Totta on, että pari kuukautta tästä
näytäntövuodesta vielä on kulumatta; mutta me epäilemme,
tulevatko ne repertoaria suuresti rikastuttamaan. Åhmanilla näemme
seuraavat klassilliset näytelmäntekijät edustettuina: Shakespeare 4,
Schiller 3, Molière 2, Beaumarchais 2, Holberg 1, Oehlenschläger 1,
mutta tämän vuoden repertoarissa ainoastaan yhden, Shakespearen,
2:lla näytelmällä. Hyvistä ulkomaan kirjailijoista oli Åhmanin
repertoarissa: Björnstjerne-Björnson (2), Musset (2), Legouvé (2),
Banville (1), Sardou (2), Augier (1), Mosenthal (1), Brachvogel (1),
Börjesson (2); kuinka kuivalta näyttää sen rinnalla tämän vuoden
repertoari, jossa tavataan: Sardou (1), Björnstjerne-Björnson (1),
Grillparzer (1), Börjesson (1). Ei kenenkään myös sopine sanoa, että
hra Åhmanin näyttelijäseura oli köyhempi hyvistä taiteilijoista, ja
yhteisnäytteleminen nyt ja silloin tuskin sietänee vertailemista.
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  • 8. Published Titles Energy Audit of Building Systems: An Engineering Approach Moncef Krarti Entropy Generation Minimization Adrian Bejan Finite Element Method Using MATLAB, 2nd Edition Young W. Kwon & Hyochoong Bang Fundamentals of Environmental Discharge Modeling Lorin R. Davis Introductory Finite Element Method Chandrakant S. Desai & Tribikram Kundu Intelligent Transportation Systems: New Principles and Architectures Sumit Ghosh & Tony Lee Mathematical & Physical Modeling of Materials Processing Operations Olusegun Johnson Ileghus, Manabu Iguchi & Walter E. Wahnsiedler Mechanics of Composite Materials Autar K. Kaw Mechanics of Fatigue Vladimir V. Bolotin Mechanism Design: Enumeration of Kinematic Structures According to Function Lung-Wen Tsai Nonlinear Analysis of Structures M. Sathyamoorthy Practical Inverse Analysis in Engineering David M. Trujillo & Henry R. Busby Principles of Solid Mechanics Rowland Richards, Jr. Thermodynamics for Engineers Kau-Fui Wong Viscoelastic Solids Roderic S. Lakes Forthcoming Titles Distributed Generation: The Power Paradigm for the New Millennium Anne-Marie Borbely & Jan F. Kreider Engineering Experimentation Euan Somerscales Fluid Power Circuits and Control: Fundamentals and Applications John S. Cundiff Heat Transfer in Single and Multiphase Systems Greg F. Naterer Mechanics of Solids & Shells Gerald Wempner & Demosthenes Talaslidis Mechanical Engineering Series Frank Kreith - Series Editor
  • 9. Chandrakant S. Desai Tribikram Kundu FINITEELEMENT METHOD Introductory Boca Raton London New York Washington, D.C. CRC Press
  • 10. This book contains information obtained from authentic and highly regarded sources. Reprinted material is quoted with permission, and sources are indicated. A wide variety of references are listed. Reasonable efforts have been made to publish reliable data and information, but the author and the publisher cannot assume responsibility for the validity of all materials or for the consequences of their use. Neither this book nor any part may be reproduced or transmitted in any form or by any means, electronic or mechanical, including photocopying, microfilming, and recording, or by any information storage or retrieval system, without prior permission in writing from the publisher. The consent of CRC Press LLC does not extend to copying for general distribution, for promotion, for creating new works, or for resale. Specific permission must be obtained in writing from CRC Press LLC for such copying. Direct all inquiries to CRC Press LLC, 2000 N.W. Corporate Blvd., Boca Raton, Florida 33431. Trademark Notice: Product or corporate names may be trademarks or registered trademarks, and are used only for identification and explanation, without intent to infringe. Visit the CRC Press Web site at www.crcpress.com © 2001 by CRC Press LLC No claim to original U.S. Government works International Standard Book Number 0-8493-0243-9 Library of Congress Card Number 2001017466 Printed in the United States of America 1 2 3 4 5 6 7 8 9 0 Printed on acid-free paper Library of Congress Cataloging-in-Publication Data Desai, C. S. (Chandrakant S.), 1936- Introductory finite element method / Chandrakant S. Desai, Tribikram Kundu. p. cm. Includes bibliographical references and index. ISBN 0-8493-0243-9 (alk. paper) 1. Finite element method. I. Kundu, T. (Tribikram). II. Title. TA347.F5 .D48 2001 620′.001′1535--dc21 2001017466 0618fm/frame Page 4 Wednesday, April 11, 2001 9:27 AM
  • 11. Dedication To Our wives: Patricia Desai and Nupur Kundu Children: Maya and Sanjay; Ina and Auni and Parents: Sankalchand Desai and Kamala Desai; Makhan Lal Kundu and Sandhya Rani Kundu 0618fm/frame Page 5 Wednesday, April 11, 2001 9:27 AM
  • 12. 0618fm/frame Page 6 Wednesday, April 11, 2001 9:27 AM
  • 13. Preface The finite element method has gained tremendous attention and popularity. The method is now taught at most universities and colleges, is researched extensively, and is used by the practicing engineers, industry, and government agencies. The teaching of the method has been concentrated at the postgrad- uate level. In view of the growth and wide use of the method, however, it becomes highly desirable and necessary to teach it at the undergraduate level. There are a number of books and publications available on the finite ele- ment method. It appears that almost all of them are suitable for the advanced students and require a number of prerequisites such as theories of constitu- tive or stress-strain laws, mechanics, and variational calculus. Some of the introductory treatments have presented the method as an extension of matrix methods of structural analysis. This viewpoint may no longer be necessary, since the finite element method has reached a significant level of maturity and generality. It has acquired a sound theoretical basis, and in itself has been established as a general procedure relevant to engineering and mathematical physics. These developments permit its teaching and use as a general tech- nique from which applications to topics such as mechanics, structures, geo- mechanics, hydraulics, and environmental engineering arise as special cases. It is therefore essential that the method be treated as a general procedure and taught as such. This book is intended mainly for the undergraduate and beginning gradu- ate students. Its approach is sufficiently elementary so that it can be intro- duced with the background of essentially undergraduate subjects. At the same time, the treatment is broad enough so that the reader or the teacher interested in various topics such as stress-deformation analysis, fluid and heat flow, potential flow, time-dependent problems, diffusion, torsion, and wave propagation can use and teach from it. The book brings out the intrinsic nature of the method that permits confluence of various disciplines and pro- vides a distinct and rather novel approach for teaching the finite element method at an elementary level. The book can be used for any student with no prior exposure to the finite element method. The prerequisites for under- standing the material will be undergraduate mathematics, strength of mate- rials, and undergraduate courses in structures, hydraulics, geotechnical engineering, and matrix algebra. Introductory knowledge of computer pro- gramming is desirable but not necessary. The text is written in such a way that no prior knowledge of variational principles is necessary. Over a period of the last 30 years or so, the authors have taught, based on these prerequi- sites, an undergraduate course and a course for user groups composed of beginners. This experience has shown that undergraduates or beginners 0618fm/frame Page 7 Wednesday, April 11, 2001 9:27 AM
  • 14. equipped with these prerequisites, available to them in the undergraduate curricula at most academic institutions, can understand and use the material presented in this book. The first chapter presents a rather philosophical discussion of the finite ele- ment method and often defines various terms on the basis of eastern and western concepts from antiquity. The second chapter gives a description of the eight basic steps and fundamental principles of variational calculus. Chapters 3 to 5 cover one-dimensional problems in stress-deformation anal- ysis and steady and time-dependent flow of heat and fluids. The fundamen- tal generality of the method is illustrated by showing the common characteristics of the formulation for these topics and by indicating the fact that their governing equations are essentially similar. The generality is fur- ther established by including computer codes in Chapter 6 that can solve dif- ferent types of problems. Understanding and using the finite element method are closely linked with the use of the computer. It is the belief of the authors that strictly theoretical teaching of the method may not give the student an idea of the details and the ranges of applicability of the technique. Consequently this text endeavors to introduce the student, gradually and simultaneously with the theoretical teaching, to the use and understanding of computer codes. The codes pre- sented in Chapter 6 are thoroughly documented and detailed so that they can be used and understood without difficulty. Details of these codes, designed for the beginner, are given in Appendix 3. It is recommended that these or other available codes be used by the student while learning various topics in this book. Chapter 7 introduces the idea of higher-order approximation for the problem of beam bending and beam-column. One-dimensional problems in mass trans- port (diffusion-convection) and wave propagation are covered in Chapters 8 and 9, respectively. These problems illustrate, by following the general proce- dure, formulations for different categories of time-dependent problems. Chapter 10 presents the basic finite element formulation for two- and three- dimensional problems. Then in Chapters 11 to 14 different types of two- dimensional problems are presented. The chapters on Torsion (Chapter 11) and Other Field Problems (Chapter 12) have been chosen because they involve only one degree-of-freedom at a point. Chapters 13 and 14 cover two- dimensional stress-deformation problems involving two and higher degrees- of-freedom at a point. The text presents the finite element method by using simple problems. It must be understood, however, that it is for the sake of easy introduction that we have used relatively simple problems. The main thrust of the method, on the other hand, is for solving complex problems that cannot be easily solved by the conventional procedures. For a thorough understanding of the finite element method, it is essential that the students perform hand calculations. With this in mind, most chapters include a number of problems to be solved by hand calculations. They also include problems for home assignments and self-study. 0618fm/frame Page 8 Wednesday, April 11, 2001 9:27 AM
  • 15. The formulations have been presented by using both the variational and residual procedures. In the former, the potential, complementary, hybrid, and mixed procedures have been discussed. In the residual procedures, main attention has been given to Galerkin’s method. A number of other residual methods are also becoming popular. They are described, therefore, in Appendix 1, which gives descriptions, solutions, and comparisons for a problem by using a number of methods: closed-form, Galerkin, collocation, subdomain, least squares, Ritz, finite difference, and finite element. Formulations by the finite element method usually result in algebraic simultaneous equations. Detailed description of these methods is beyond the scope of this book. Included in Appendix 2, however, are brief introductions to the commonly used direct and iterative procedures for the solution of alge- braic simultaneous equations. Appendix 3 presents details of a number of computer codes relevant to var- ious topics in the text. The book can be used for one or two undergraduate courses. The second course may overlap with or be an introductory graduate course. Although a number of topics have been covered in the book, a semester or quarter course could include a selected number of topics. For instance, a quarter course can cover Chapters 1 to 6, and then one or two topics from the remaining chapters. For a class interested in mechanics and stress-deforma- tion analyses, the topics can be Beam Bending and Beam-Column (Chapter 7), and Two-Dimensional Stress Deformation (Chapters 10 and 13). If time is available (in the case of a semester course), Chapter 9 on One- Dimensional Stress Wave Propagation, Chapter 11 on Torsion, and/or Chapter 14 on Multicomponent Systems can be added. A class oriented toward field problems and hydraulics can choose one or more of Chapters 8, 9, 11, and 12 in addition to Chapters 1 to 6 and 10. We would like to express special appreciation to Jose Franscisco Perez Avila for his assistance in the manuscript preparation and Shashank Pradhan for implementing some of the computer codes and preparation of user’s manuals. We realize that it is not easy to write at an elementary level for the finite ele- ment method with so many auxiliary disciplines. The judgment of this book is better left to the readers. Many natural systems can be considered continuous or interconnected, and their behavior is influenced by a large number of parameters. In order to understand such a system, we must understand all the parameters. Since this is not possible we make approximations, by selecting only the significant of them and neglecting the others. Such a procedure allows understanding of the entire system by comprehending its components taken one at a time. These approximations or models obviously involve errors, and we strive con- tinuously to improve the models and reduce the errors. Chandrakant S. Desai Tribikram Kundu Tucson, Arizona 0618fm/frame Page 9 Wednesday, April 11, 2001 9:27 AM
  • 16. 0618fm/frame Page 6 Wednesday, April 11, 2001 9:27 AM
  • 17. Authors Chandrakant S. Desai is a Regents’ Profes- sor and Director of the Material Modeling and Computational Mechanics Center, Department of Civil Engineering and Engi- neering Mechanics, University of Arizona, Tucson. He was a Professor in the Depart- ment of Civil Engineering, Virginia Poly- technic Institute and State University, Blacksburg, from 1974 to 1981, and a Research Civil Engineer at the U.S. Army Engineer Waterways Experiment Station, Vicksburg, MS from 1968 to 1974. Dr. Desai has made original and signifi- cant contributions in basic and applied research in material modeling and testing, and computational methods for a wide range of problems in civil engineering, mechanics, mechanical engineering, and electronic packaging. He has authored/edited 20 books and 18 book chap- ters, and has been the author/coauthor of over 270 technical papers. He was the founder and General Editor of the International Journal for Numerical and Analytical Methods in Geomechanics from 1977 to 2000, and he has served as a member of the editorial boards of 12 journals. Dr. Desai has also been a chair/member of a number of committees of var- ious national and international societies. He is the President of the Interna- tional Association for Computer Methods and Advances in Geomechanics. Dr. Desai has also received a number of recognitions: Meritorious Civilian Service Award by the U.S. Corps of Engineers, Alexander von Humboldt Stif- tung Prize by the German Government, Outstanding Contributions Medal in Mechanics by the International Association for Computer Methods and Advances in Geomechanics, Distinguished Contributions Medal by the Czech Academy of Sciences, Clock Award by ASME (Electrical and Electronic Packaging Division), Five Star Faculty Teaching Finalist Award, and the El Paso Natural Gas Foundation Faculty Achievement Award at the Univer- sity of Arizona, Tucson. 0618fm/frame Page 11 Wednesday, April 11, 2001 9:27 AM
  • 18. Professor T. Kundu received his bachelor degree in mechanical engineering from the Indian Institute of Technology, Kharagpur in 1979. His M.S. and Ph.D. were in the field of mechanics from the Mechanical and Aerospace Engineering Department of the University of California, Los Angeles in 1980 and 1983, respectively. He joined the University of Arizona as an assistant pro- fessor in 1983 and was promoted to full professor in 1994. Dr. Kundu has made significant and orig- inal contributions in both basic and applied research in computational mechanics and nondestructive evaluation (NDE) of mate- rials by ultrasonic and acoustic microscopy techniques. He is editor or coeditor of 8 books, coauthor of a textbook, author of a book chapter, and author/coauthor of over 130 technical papers; half of those have been published in refereed journals. He is a Fellow of ASME (American Society of Mechanical Engineers) and ASCE (American Society of Civil Engineers). He has received a number of awards, including the Presi- dent’s Gold Medal from IIT, the UCLA Alumni Award, the Humboldt Fel- lowship from Germany, and the Best Paper Award from the International Society for Optical Engineering (SPIE). He has extensive research collabora- tions with international and U.S. scientists. He has spent 21 months as an Alexander von Humboldt Scholar in the Department of Biology, J. W. Goethe University, Frankfurt, Germany. He has also spent several months as a visit- ing professor at a number of other institutes — Department of Mechanics, Chalmers University of Technology, Gothenberg, Sweden; Acoustic Micros- copy Center, Semienov Institute of Chemical Physics, Russian Academy of Science, Moscow; Department of Civil Engineering, EPFL (Swiss Federal Institute of Technology in Lausanne), Switzerland; Department of Mechani- cal Engineering, University of Technology of Compiegne, France; Materials Laboratory, University of Bordeaux, France; LESiR Laboratory, Ecole Nor- male Superior (ENS), Cachan, France; Aarhus University Medical School, Aarhus, Denmark; Wright-Patterson Material Laboratory, Dayton, OH. 0618fm/frame Page 12 Wednesday, April 11, 2001 9:27 AM
  • 19. Contents 1 Introduction ..................................................................................... 1 Basic Concept...........................................................................................................1 Process of Discretization ........................................................................................3 Subdivision .....................................................................................................3 Continuity .......................................................................................................4 Convergence ...................................................................................................4 Bounds.............................................................................................................5 Error .................................................................................................................6 Principles and Laws................................................................................................7 Cause and Effect....................................................................................................10 Important Comment....................................................................................10 Review Assignments ............................................................................................10 Home Assignment 1 .................................................................................... 11 Home Assignment 2 ....................................................................................12 References ............................................................................................... 12 2 Steps in the Finite Element Method ............................................ 13 Introduction ...........................................................................................................13 General Idea...........................................................................................................13 Step 1. Discretize and Select Element Configuration.................14 Step 2. Select Approximation Models or Functions...................16 Step 3. Define Strain (Gradient)-Displacement (Unknown) and Stress–Strain (Constitutive) Relationships .............18 Step 4. Derive Element Equations ................................................19 Energy Methods ...........................................................................................19 Stationary Value ...........................................................................................20 Potential Energy...........................................................................................20 Method of Weighted Residuals..................................................................22 Element Equations .......................................................................................25 Step 5. Assemble Element Equations to Obtain Global or Assemblage Equations and Introduce Boundary Conditions ..........................................................................26 Boundary Conditions ..................................................................................27 Step 6. Solve for the Primary Unknowns ....................................29 Step 7. Solve for Derived or Secondary Quantities....................29 Step 8. Interpretation of Results....................................................29 Introduction to Variational Calculus..................................................................30 Definitions of Functions and Functionals.................................................30 Variations of Functions................................................................................31 Stationary Values of Functions and Functionals .........................36 0618fm/frame Page 13 Wednesday, April 11, 2001 9:27 AM
  • 20. ∆fx to ∆f Conversion .....................................................................................37 More on the Stationary Value of a Functional — Physical Interpretation....................................................................................38 Natural and Forced Boundary Conditions...............................................39 Two-Dimensional Problems .......................................................................41 Summary ................................................................................................................47 Problems.................................................................................................................48 References ............................................................................................... 50 3 One-Dimensional Stress Deformation ........................................ 53 Introduction ...........................................................................................................53 Step 1. Discretization and Choice of Element Configuration .....................................................................53 Explanation of Global and Local Coordinates..................................................54 Local and Global Coordinate System for the One-Dimensional Problem .....55 Step 2. Select Approximation Model or Function for the Unknown (Displacement)....................................56 Generalized Coordinates ............................................................................57 Interpolation Functions........................................................................................60 Relation between Local and Global Coordinates .............................................61 Variation of Element Properties.................................................................61 Requirements for Approximation Functions ....................................................62 Step 3. Define Strain-Displacement and Stress–Strain Relations..............................................................................64 Stress–Strain Relation...........................................................................................65 Step 4. Derive Element Equations ................................................66 Principle of Minimum Potential Energy............................................................66 Functional for One-Dimensional Stress Deformation Problem ............69 Total Potential Energy Approach...................................................69 Variational Principle Approach......................................................71 Expansion of Terms...............................................................................................73 Integration..............................................................................................................75 Comment.......................................................................................................77 Step 5. Assemble Element Equations to Obtain Global Equations ............................................................................77 Direct Stiffness Method........................................................................................80 Boundary Conditions ...........................................................................................82 Types of Boundary Conditions ..................................................................83 Homogeneous or Zero-Valued Boundary Condition .............................83 Nonzero Boundary Conditions..................................................................84 Step 6. Solve for Primary Unknowns: Nodal Displacements ....................................................................85 Step 7. Solve for Secondary Unknowns; Strains and Stresses ................................................................................88 Strains and Stresses...............................................................................................88 Step 8. Interpretation and Display of Results .............................90 0618fm/frame Page 14 Wednesday, April 11, 2001 9:27 AM
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  • 22. [18] Vrt. Schillerin omaa kirjoitusta "Briefe über Don Carlos". [19] Vrt. Schiller und seine Zeitgen. von J. Schmidt, s. 379-427. Schiller von K. Grün, s. 682-704. [20] Vrt. Geschichte der deutschen Litteratur seit Lessings Tod von J. Schmidt, s. 224. Friedr. Schiller von K. Grün, s, 704-716. [21] Vrt. Schiller und seine Zeitgen. von J. Schmidt, s. 435-441, Gesch. der deut. Litterat, von J. Schmidt, II, s. 251-254. Friedr. Schiller von K. Grün, s. 716-736. Oldenb. Theaterschau von Stahr, s. 101-120. Schillers Dichtungen von Hinrichs, s. 180-237. [22] Schiller und seine Zeitgen. von J. Schmidt, s. 453-458. Geschichte der deutschen Litter. seit Lessings Tod von J. Schmidt, s. 379-381. Friedr. Schiller von K. Grün, s. 754-772. Schillers Dichtungen von Hinrichs, s. 278-314. Die romantische Schule in ihrem Zusammenhange mit Goethe und Schiller von Hettner, s. 122- 131. [23] Vrt. tähän esitykseen Geschichte der deutschen Literatur seit Lessings Tod von Julian Schmidt, II. Die romantische Schule in ihrem inneren Zusammenhange mit Goethe und Schiller von Herman Hettner. [24] Vrt. Gesch. der deut. Litter. seit Lessings Tod von J. Schmidt, s. 301, 446, 518. III 14. Neure Geschichte der poetischen Nationalliteratur von Gervinus, II s. 595, 668. Die deutsche Nationallitteratur in der ersten Hälfte des 19:n Jahrhunderts von E. Gottschall, I s. 164 ja seur.
  • 23. [25] Gesch. der deut. Literatur von J. Schmidt II s. 564. Die deutsche Nationallit. in der ersten Hälfte der 19:n Jahrhunderts von Gottschall, I s. 317. [26] Vrt. Gesch. der deutsch. Litter. seit Lessings Tod von J. Schmidt, III s. 27. Die deutsche Nationallit. in der ersten Hälfte des 19:n Jahrh. von Gottschall, I s. 296. [27] Vrt. Kleistin "Sämmtliche Schriften'in" esipuhetta, jonka Tieck ja J. Schmidt ovat kirjoittaneet. Gesch. der deut. Liter, seit Lessings Tod von J. Schmidt, II s. 325, 569, 597. Die deut. Nationallit. in der ersten Hälfte des 19:n Jahrh. von R. Gottschall, II s. 320. [28] Niin oli tosin laita vielä 19:nnen vuosisadan keskivaiheilla mutta sen loppupuolella on Kleist tullut sitä suuremman huomion ja tunnustuksen esineeksi. (Kääntäjän muist.) [29] "Minussa herätti Kleist, vaikka puhtain tarkoitukseni oli vilpitön osanotto, vain kauhua ja inhoa, niinkuin luonnon puolesta kauniiksi aiottu ruumis, jota kalvaa parantumaton tauti." [30] Die deutsche Nationalliteratur in der ersten Hälfte des 19:n Jahrhunderts von R. Gottschall, I s. 302. [31] Vrt. Die Dramatiker der Jetz-zeit von L. Wienbarg, I. Ludwig Mand, sein Leben und seine Dichtungen von F. Nötter, s. 432. [32] Vrt. Die deutsche Nationallit. in der ersten Hälfte des 19:n Jahrh. von R. Gottschall, I s. 184. [33] Teoksessaan "Dramaturgische Blätter".
  • 24. [34] Vrt. Die deutsche Nationallit. in der ersten Hälfte des 19:n Jahrh. von R. Gottschall, II s. 398. [35] Vrt. Die deutsche Nationallit. in der ersten Hälfte des 19:n Jahrh. von R. Gottschall, II s. 414. [36] Niin on Immermann kritiseerannut, korjannut, karrikeerannut esim. Gryphiuksen "Oardeniota ja Celindeä" samannimisessä tragediassaan, Goethen "Tassoa" "Petrarcassaan", Goethen "Faustia" "Merlinissään", Goethen "Wilhelm Meisteria" romaanissaan "Die Epigonen", Schillerin "Don Carlosta" "Alexissaan", Schillerin "Wilhelm Telliä" näytelmässään "Trauerspiel im Tyrol" j.n.e. [37] Vrt. Willkomin kirjoittamaa luonteenkuvausta Grabbesta teoksessa "Jahrbücher für Drama, Dramaturgie und Theater" I. Grabbes Leben von Ed. Duller. Die deutsche Nationalliter. von GottschaH II s. 334. [38] Vrt. Gesch. der deutschen Litt. von Schmidt, III s 252. Die deutsche Nationallit. in der ersten Hälfte des 19:n Jahrh. von Gottschall, II s. 367. [39] Vrt. Das deutsche Drama der Gegenwart von A. Henneberger, s. 24. [40] Vrt. Das deutsche Drama der Gegenwart von Henneberger, s. 36. Die deutsche Nationallit. von Gottschall, II s. 454. Die Geschichte der deutschen Nationallit. von J. Schmidt, III s. 348.
  • 25. [41] Das deutsche Drama der Gegenwart von Henneberger, s. 53. Die deutsche Nationallit. von Gottschall, II. s. 461. [42] Das deutsche Drama der Gegenwart von Henneberger s. 12. Die deutsche Nationallit. von R. Gottsohall, II s. 470. [43] Das deutsche Drama der Gegenwart von Henneberger, s. 21. Oldenburgischer Teatersohau von A. Stahr, I s. 214, 238, 258. II s. 94, 125. [44] Paitsi näitä novelleja on myös "Arbetets ära" ("Työn kunnia") käännetty suomeksi. Myöhemmin myös kertomus "Araminta May". [45] V. Löfgrenin suomentamina. [46] Jos tahtoo verrata, mimmoinen taiteellisten tarkoitusten ohjaama teatterinjohto on käsityöntapaiseen verrattuna, asetettakoon rinnakkain Åhmanin teatteriseuran repertoari täällä vuonna 1866-67 ja nykyinen. Totta on, että pari kuukautta tästä näytäntövuodesta vielä on kulumatta; mutta me epäilemme, tulevatko ne repertoaria suuresti rikastuttamaan. Åhmanilla näemme seuraavat klassilliset näytelmäntekijät edustettuina: Shakespeare 4, Schiller 3, Molière 2, Beaumarchais 2, Holberg 1, Oehlenschläger 1, mutta tämän vuoden repertoarissa ainoastaan yhden, Shakespearen, 2:lla näytelmällä. Hyvistä ulkomaan kirjailijoista oli Åhmanin repertoarissa: Björnstjerne-Björnson (2), Musset (2), Legouvé (2), Banville (1), Sardou (2), Augier (1), Mosenthal (1), Brachvogel (1), Börjesson (2); kuinka kuivalta näyttää sen rinnalla tämän vuoden repertoari, jossa tavataan: Sardou (1), Björnstjerne-Björnson (1), Grillparzer (1), Börjesson (1). Ei kenenkään myös sopine sanoa, että hra Åhmanin näyttelijäseura oli köyhempi hyvistä taiteilijoista, ja yhteisnäytteleminen nyt ja silloin tuskin sietänee vertailemista.
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