Preface
Mechanics is, of course, the study of how things move --- how an
electron moves down your TV tube, how a baseball flies through the air,
how a comet moves round the sun. Classical mechanics is the form of
mechanics developed by Galileo and Newton in the seventeenth century and
reformulated by Lagrange and Hamilton in the eighteenth and nineteenth
centuries. For almost three hundred years, it seemed that classical
mechanics was the form of mechanics, that it could explain
the motion of all conceivable systems. Then, in two great revolutions
of the early twentieth century it was shown that classical mechanics
cannot account for the motion of objects traveling close to the speed of
light, nor of subatomic particles moving inside atoms. The years from
about 1900 to 1930 saw the development of relativistic mechanics
primarily to describe fast moving bodies and of quantum mechanics
primarily to describe subatomic systems. Faced with this competition,
one might expect classical mechanics to have lost much of its interest
and importance. In fact, however, classical mechanics is now, at the
start of the twenty-first century, just as important and glamorous as
ever. This resilience is due to two facts: First, there are just as
many interesting physical systems as ever that are best described in
classical terms. To understand the orbits of space vehicles and of
charged particles in modern accelerators, you have to understand
classical mechanics. Second, recent developments in classical
mechanics, mainly associated with the growth of chaos theory, have
spawned whole new branches of physics and mathematics and have changed
our understanding of the notion of causality. It is these new ideas
that have attracted some of the best minds in physics back to the study
of classical mechanics.
Physicists tend to use the term ``classical mechanics'' rather loosely.
Many use it for the mechanics of Newton, Lagrange, and Hamilton, and for these people, ``classical mechanics'' excludes relativity and quantum
mechanics. On the other hand, in some areas of physics, there is a
tendency to include relativity as a part of ``classical mechanics''; for
people of this persuasion, ``classical mechanics'' means ``non-quantum
mechanics.'' Perhaps as a reflection of this second usage, some courses
called ``classical mechanics'' include an introduction to relativity,
and for the same reason, I have included one chapter on relativistic
mechanics, which you can use or not, as you please.
An attractive feature of a course in classical mechanics is that it is a
wonderful opportunity to learn to use many of the mathematical
techniques needed in so many other branches of physics --- vectors,
vector calculus, differential equations, complex numbers, Taylor series,
Fourier series, calculus of variations, and matrices. I have tried to
give at least a minimal review or introduction for each of these topics
(with references to further reading) and to teach their use in the
usually quite simple context of classical mechanics. I hope you will
come away from this book with an increased confidence that you can really use these important tools.
Inevitably, there is more material in the book than could possibly be
covered in a one-semester course. I have tried to ease the pain of
choosing what to omit. A number of sections are marked with an asterisk
to indicate that they can be omitted without loss of continuity. (This
is not to say that this material is unimportant. I certainly hope
you'll come back and read it later!) And the last seven chapters are
designed to be mutually independent, so that you can choose to read any
one of them without reference to any of the others.
As always in a physics text, it is crucial that you do lots of the
exercises at the end of each chapter. I have included a large number of
these to give both teacher and student plenty of choice. Some of them
are simple applications of the ideas of the chapter and some are
extensions of those ideas. I have listed the problems by section, so
that as soon as you have read any given section you could (and probably
should) try a few problems listed for that section. (Naturally,
problems listed for a given section may require knowledge of earlier
sections. I promise only that you shouldn't need material from later
sections.) I have tried to grade the problems to indicate their level
of difficulty, ranging from one star,\st, (meaning a straightforward
exercise usually involving just one main concept) to three stars,\ssst,
(meaning a challenging problem that involves several concepts and will
probably take considerable time and effort). This kind of
classification is quite subjective and is necessarily only very
approximate. Several of the problems require the use of computers to
plot graphs, solve differential equations, and so on. None of these
requires any specific software; some can be done with a relatively
simple system such as MathCad; some require more sophisticated systems,
such as Mathematica, Maple, or Matlab. (Incidentally it is my experience
that the course for which this book was written is a wonderful
opportunity for the students to learn to use one of these fabulously
useful systems.) Problems requiring the use of a computer are indicated
thus: [Computer]. I have tended to grade them as \ssst, or at least
\sst, on the grounds that it takes time to set up the necessary code.
Naturally, these problems will be easier for students who are
experienced with the necessary software.
There are many people I wish to thank for their help and suggestions.
At the University of Colorado, these include Professors John Cox, Scott
Parker, Steve Pollock, Mike Dubson, Mike Ritzwoller, and Larry Baggett.
From other institutions, I want to thank the following: Professors E.
Stern at the University of Washington, John Markert and Tom Griffy at
the University of Texas, R. Pompi at SUNY at Binghampton, Meagan Aronson
at the University of Michigan, and Peter Blunden at the University of
Manitoba. I particularly want to thank my two friends and colleagues,
Dave Goodmanson at the Boeing Aircraft Company and Mark Semon at Bates
College, who both reviewed the manuscript with the finest of combs and
gave me literally hundreds of suggestions; for their help and advice I
am especially grateful. Bruce Armbruster and Jane Ellis of University
Science Books are an author's dream come true. Finally and most of all,
I want to thank my wife Debby. Being married to an author can be quite
trying, and she puts up with it very graciously. And, as an English
teacher with the highest possible standards, she has taught me most of
what I know about writing and editing. I am eternally grateful.
This preliminary edition is missing the last three chapters, and there
are some other additions and changes that I would have made if there
had been more time. For example, I fully intend to add some more
end-of-chapter problems to some of the later chapters. The purpose of
this preliminary edition is to find ways to improve the book before its
official launch. All suggestions, both large and small, will be most
welcome.
The first two questions about any text book are: ``What is it
about?'' and ``For what audience is it intended.'' The brief answer to the first
question is that this book is about classical mechanics --- a subject
I'll describe in a moment. The answer to the second is that this book
is intended for students of the physical sciences, especially physics,
who have already met mechanics as part of an introductory physics course
(``freshman physics'' at a typical American university) and are now
ready for a deeper look at the subject. The book grew out of the
junior-level mechanics course which is offered by the Physics Department
at Colorado and is taken mainly by physics majors, but also by some
mathematicians, chemists, and engineers. Almost all of these students
have taken a year of freshman physics, and so have at least a nodding
acquaintance with Newton's laws, energy and momentum, simple harmonic
motion, and so on. In this book I build on this nodding acquaintance to
give a deeper understanding of these basic ideas, and then go on to
develop more advanced topics, such as the Lagrangian and Hamiltonian
formulations, the mechanics of non-inertial frames, motion of rigid
bodies, coupled oscillators, chaos theory, and a few more.
John R. Taylor
University of Colorado
Boulder, Colorado 80309
John.Taylor@Colorado.edu
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