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C M lassical echanics 5th Edition C lassical M echanics 5th Edition Tom W.B. Kibble Frank H. Berkshire Imperial College London Imperial College Press ICP Published by Imperial College Press 57 Shelton Street Covent Garden London WC2H 9HE Distributed by World Scientific Publishing Co. Pte. Ltd. 5 Toh Tuck Link, Singapore 596224 USA office: Suite 202, 1060 Main Street, River Edge, NJ 07661 UK office: 57 Shelton Street, Covent Garden, London WC2H 9HE Library of Congress Cataloging-in-Publication Data Kibble, T. W. B. Classical mechanics / Tom W. B. Kibble, Frank H. Berkshire, -- 5th ed. p. cm. Includes bibliographical references and index. ISBN 1860944248 -- ISBN 1860944353 (pbk). 1. Mechanics, Analytic. I. Berkshire, F. H. (Frank H.). II. Title QA805 .K5 2004 531'.01'515--dc 22 2004044010 British Library Cataloguing-in-Publication Data A catalogue record for this book is available from the British Library. Copyright © 2004 by Imperial College Press All rights reserved. This book, or parts thereof, may not be reproduced in any form or by any means, electronic or mechanical, including photocopying, recording or any information storage and retrieval system now known or to be invented, without written permission from the Publisher. For photocopying of material in this volume, please pay a copying fee through the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, USA. In this case permission to photocopy is not required from the publisher. Printed in Singapore. To Anne and Rosie vi Preface Thisbook,basedoncoursesgiventophysicsandappliedmathematicsstu- dents at Imperial College, deals with the mechanics of particles and rigid bodies. It is designed for students with some previous acquaintance with theelementaryconceptsofmechanics,butthebookstartsfromfirstprinci- ples,andlittledetailedknowledgeisassumed. Anessentialprerequisiteisa reasonablefamiliaritywithdifferentialandintegralcalculus,includingpar- tial differentiation. However, no prior knowledge of differential equations should be needed. Vectors are used from the start in the text itself; the necessarydefinitionsandmathematicalresultsarecollectedinanappendix. Classicalmechanicsisaveryoldsubject. Its basicprincipleshavebeen known since the time of Newton, when they were formulated in the Prin- cipia, and the mathematical structure reached its mature form with the worksofLagrangeinthelateeighteenthcenturyandHamiltoninthenine- teenth. Remarkably enough, within the last few decades the subject has once again become the focus of very active fundamental research. Some of the most modern mathematical tools have been brought to bear on the problem of understanding the qualitative features of dynamics, in particu- larthetransitionbetweenregularandturbulentorchaoticbehaviour. The fourthedition ofthe book wasextended to include newchaptersproviding abriefintroductiontothisexcitingwork. Inthisfifthedition,thematerial issomewhatexpanded,inparticulartocontrastcontinuousanddiscretebe- haviours. Wehavealsotakentheopportunitytorevisetheearlierchapters, giving more emphasis to specific examples workedout in more detail. Manyofthemostfascinatingrecentdiscoveriesaboutthenatureofthe Earth and its surroundings — particularly since the launching of artificial satellites — are direct applications of classicalmechanics. Severalof these are discussed in the following chapters, or in problems. vii viii ClassicalMechanics For physicists, however, the real importance of classical mechanics lies notsomuchinthevastrangeofitsapplicationsasinitsroleasthebaseon which the whole pyramid of modern physics has been erected. This book, therefore,emphasizesthose aspects ofthe subjectwhichareof importance inquantummechanicsandrelativity—particularlytheconservationlaws, which in one form or another play a central role in all physicaltheories. For applied mathematicians, the methods of classical mechanics have evolved into a much broader theory of dynamical systems with many ap- plications well outside of physics, for example to biologicalsystems. The first five chapters areprimarily concernedwith the mechanics of a singleparticle,andChapter6,whichcouldbeomittedwithoutsubstantially affecting the remaining chapters, deals with potential theory. Systems of particles arediscussed in Chapters 7 and 8, and rigidbodies in Chapter 9. ThepowerfulmethodsofLagrangeareintroducedatanearlystage,andin simplecontexts,anddevelopedmorefully inChapters10and11. Chapter 12 contains a discussion of Hamiltonian mechanics, emphasizing the rela- tionship between symmetries and conservation laws — a subject directly relevant to the most modern developments in physics. It also provides the basis for the later treatment of order and chaos in Hamiltonian systems in Chapter14. Thisfollowstheintroductiontothegeometricaldescriptionof continuous dynamical systems in Chapter 13, which includes a discussion ofvariousnon-mechanicsapplications. Appendices fromthe fourthedition on (A) Vectors, (B) Conics, (C) Phase-plane analysis near critical points aresupplemented hereby a newappendix (D) Discrete dynamicalsystems — maps. Thewritingofthefirsteditionofthisbookowedmuchtotheadviceand encouragement of the late Professor P.T. Matthews. Several readers have alsohelpedbypointingouterrors,particularlyintheanswerstoproblems. We are grateful to the following for permission to reproduce copyright material: Springer–VerlagandProfessorOscarE.LanfordIIIforFig.13.20; Cambridge University Press for Fig. 13.22 and, together with Professors G.L. Baker and J.P. Gollub, for Fig. D.5; Institute of Physics Publishing Limited and Professor M.V. Berry for Figs. 14.11, 14.12 and 14.13; the RoyalSociety and ProfessorsW.P. Reinhardtand I.Dana for the figurein the answer to Appendix D, Problem 13. T.W.B. Kibble F.H. Berkshire Imperial College London Contents Preface vii Useful Constants and Units xv List of Symbols xvii 1. Introduction 1 1.1 Space and Time . . . . . . . . . . . . . . . . . . . . . . . 2 1.2 Newton’s Laws . . . . . . . . . . . . . . . . . . . . . . . . 5 1.3 The Concepts of Mass and Force . . . . . . . . . . . . . . 10 1.4 External Forces . . . . . . . . . . . . . . . . . . . . . . . 13 1.5 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . 13 2. Linear Motion 17 2.1 Conservative Forces; Conservationof Energy . . . . . . . 17 2.2 Motion near Equilibrium; the Harmonic Oscillator . . . . 20 2.3 Complex Representation . . . . . . . . . . . . . . . . . . 24 2.4 The Lawof Conservationof Energy . . . . . . . . . . . . 25 2.5 The Damped Oscillator . . . . . . . . . . . . . . . . . . . 27 2.6 Oscillator under Simple PeriodicForce . . . . . . . . . . 30 2.7 General Periodic Force . . . . . . . . . . . . . . . . . . . 34 2.8 Impulsive Forces; the Green’s Function Method . . . . . 37 2.9 Collision Problems. . . . . . . . . . . . . . . . . . . . . . 39 2.10 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . 42 ix

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