Introduction To Classical Mechanics With Problems And Solutions

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Introduction to Classical MechanicsWith Problems and SolutionsThis textbook covers all the standard introductory topics in classical mechanics,including Newton’s laws, oscillations, energy, momentum, angular momentum,planetary motion, and special relativity. It also explores more advanced topics,such as normal modes, the Lagrangian method, gyroscopic motion, fictitiousforces, 4-vectors, and general relativity.It contains more than 250 problems with detailed solutions so students caneasily check their understanding of the topic. There are also over 350 unworkedexercises, which are ideal for homework assignments. Password-protectedsolutions are available to instructors at www.cambridge.org/9780521876223.The vast number of problems alone makes it an ideal supplementary book forall levels of undergraduate physics courses in classical mechanics. The text alsoincludes many additional remarks which discuss issues that are often glossedover in other textbooks, and it is thoroughly illustrated with more than 600figures to help demonstrate key concepts.David Morin is a Lecturer in Physics at Harvard University. He received hisPh.D. in theoretical particle physics from Harvard in 1996. When not writingphysics limericks or thinking of new problems whose answers involve e or thegolden ratio, he can be found running along the Charles River or hiking in theWhite Mountains of New Hampshire.MORIN: “FM” — 2007/10/9 — 19:08 — page i — #1

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Introduction to ClassicalMechanicsWith Problems and SolutionsDavid MorinHarvard UniversityMORIN: “FM” — 2007/10/9 — 19:08 — page iii — #3

Cambridge University PressCambridge, New York, Melbourne, Madrid, Cape Town, Singapore, São PauloCambridge University PressThe Edinburgh Building, Cambridge CB2 8RU, UKPublished in the United States of America by Cambridge University Press, New Yorkwww.cambridge.orgInformation on this title: www.cambridge.org/9780521876223 D. Morin 2007This publication is in copyright. Subject to statutory exceptionand to the provisions of relevant collective licensing agreements,no reproduction of any part may take place withoutthe written permission of Cambridge University Press.First published 2008Printed in the United Kingdom at the University Press, CambridgeA catalog record for this publication is available from the British LibraryISBN 978-0-521-87622-3 hardbackCambridge University Press has no responsibility for the persistence oraccuracy of URLs for external or third-party internet websites referred toin this publication, and does not guarantee that any content on suchwebsites is, or will remain, accurate or appropriate.MORIN: “FM” — 2007/10/9 — 19:08 — page iv — #4

To Allen Gerry and Neil Tame,who took the timeto give a group of kidssome really cool problemsMORIN: “FM” — 2007/10/9 — 19:08 — page v — #5

There once was a classical theory,Of which quantum disciples were leery.They said, “Why spend so longOn a theory that’s wrong?”Well, it works for your everyday query!MORIN: “FM” — 2007/10/9 — 19:08 — page vi — #6

ContentsPrefacepage xiii1 Strategies for solving problems1.1 General strategies1.2 Units, dimensional analysis1.3 Approximations, limiting cases1.4 Solving differential equations numerically1.5 Problems1.6 Exercises1.7 Solutions1147111415182 Statics2.1 Balancing forces2.2 Balancing torques2.3 Problems2.4 Exercises2.5 Solutions2222273035393 Using F ma3.1 Newton’s laws3.2 Free-body diagrams3.3 Solving differential equations3.4 Projectile motion3.5 Motion in a plane, polar coordinates3.6 Problems3.7 Exercises3.8 Solutions5151556065687075844 Oscillations4.1 Linear differential equations4.2 Simple harmonic motion101101105viiMORIN: “FM” — 2007/10/9 — 19:08 — page vii — #7

viiiContents4.34.44.54.64.74.8Damped harmonic motionDriven (and damped) harmonic motionCoupled 221275 Conservation of energy and momentum5.1 Conservation of energy in one dimension5.2 Small oscillations5.3 Conservation of energy in three dimensions5.4 Gravity5.5 Momentum5.6 The center of mass frame5.7 Collisions5.8 Inherently inelastic processes5.9 Problems5.10 Exercises5.11 Solutions1381381471481521561611641671731801946 The Lagrangian method6.1 The Euler–Lagrange equations6.2 The principle of stationary action6.3 Forces of constraint6.4 Change of coordinates6.5 Conservation laws6.6 Noether’s theorem6.7 Small oscillations6.8 Other applications6.9 Problems6.10 Exercises6.11 Solutions2182182212272292322362392422462512557 Central forces7.1 Conservation of angular momentum7.2 The effective potential7.3 Solving the equations of motion7.4 Gravity, Kepler’s laws7.5 Problems7.6 Exercises7.7 Solutions281281283285287296298300MORIN: “FM” — 2007/10/9 — 19:08 — page viii — #8

Contents8 Angular momentum, Part I (Constant L̂)8.1 Pancake object in x-y plane8.2 Nonplanar objects8.3 Calculating moments of inertia8.4 Torque8.5 Collisions8.6 Angular impulse8.7 Problems8.8 Exercises8.9 Solutions3093103163183223283313333393499 Angular momentum, Part II (General L̂)9.1 Preliminaries concerning rotations9.2 The inertia tensor9.3 Principal axes9.4 Two basic types of problems9.5 Euler’s equations9.6 Free symmetric top9.7 Heavy symmetric top9.8 Problems9.9 Exercises9.10 Solutions37137137638338839339639941542142810 Accelerating frames of reference10.1 Relating the coordinates10.2 The fictitious forces10.3 Tides10.4 Problems10.5 Exercises10.6 Solutions45745846047147748248611 Relativity (Kinematics)11.1 Motivation11.2 The postulates11.3 The fundamental effects11.4 The Lorentz transformations11.5 Velocity addition11.6 The invariant interval11.7 Minkowski diagrams11.8 The Doppler effect11.9 Rapidity11.10 Relativity without c501502509511523529533536539543546MORIN: “FM” — 2007/10/9 — 19:08 — page ix — #9ix

xContents11.11 Problems11.12 Exercises11.13 Solutions54955656512 Relativity (Dynamics)12.1 Energy and momentum12.2 Transformations of E and p12.3 Collisions and decays12.4 Particle-physics units12.5 Force12.6 Rocket motion12.7 Relativistic strings12.8 Problems12.9 Exercises12.10 Solutions58458459459660060160660961161561913 4-vectors13.1 Definition of 4-vectors13.2 Examples of 4-vectors13.3 Properties of 4-vectors13.4 Energy, momentum13.5 Force and acceleration13.6 The form of physical laws13.7 Problems13.8 Exercises13.9 Solutions63463463563763964064364564564614 General Relativity14.1 The Equivalence Principle14.2 Time dilation14.3 Uniformly accelerating frame14.4 Maximal-proper-time principle14.5 Twin paradox revisited14.6 Problems14.7 Exercises14.8 Solutions649649650653656658660663666Appendix AAppendix BAppendix CAppendix DAppendix EAppendix F675679690693696698Useful formulasMultivariable, vector calculusF ma vs. F dp/dtExistence of principal axesDiagonalizing matricesQualitative relativity questionsMORIN: “FM” — 2007/10/9 — 19:08 — page x — #10

ContentsAppendix GAppendix HAppendix IAppendix JReferencesIndexDerivations of the Lv/c2 resultResolutions to the twin paradoxLorentz transformationsPhysical constants and data704706708711713716MORIN: “FM” — 2007/10/9 — 19:08 — page xi — #11xi

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PrefaceThis book grew out of Harvard University’s honors freshman mechanics course.It is essentially two books in one. Roughly half of each chapter follows the form ofa normal textbook, consisting of text, along with exercises suitable for homeworkassignments. The other half takes the form of a “problem book,” with all sortsof problems (and solutions) of varying degrees of difficulty. I’ve always thoughtthat doing problems is the best way to learn, so if you’ve been searching for asupply to puzzle over, I think this will keep you busy for a while.This book is somewhat of a quirky one, so let me say right at the start how Iimagine it being used: As the primary text for honors freshman mechanics courses. My original motivationfor writing it was the fact that there didn’t exist a suitable book for Harvard’s freshmancourse. So after nine years of using updated versions in the class, here is the finishedproduct. As a supplementary text for standard freshman courses for physics majors. Althoughthis book starts at the beginning of mechanics and is self contained, it doesn’t spendas much time on the introductory material as other freshman books do. I thereforedon’t recommend using this as the only text for a standard freshman mechanics course.However, it will make an extremely useful supplement, both as a problem book for allstudents, and as a more advanced textbook for students who want to dive further intocertain topics. As a supplementary text for upper-level mechanics courses, or as the primary text whichis supplemented with another book for additional topics often covered in upper-levelcourses, such as Hamilton’s equations, fluids, chaos, Fourier analysis, electricity andmagnetism applications, etc. With all of the worked examples and in-depth discussions,you really can’t go wrong in pairing up this book with another one. As a problem book for anyone who likes solving physics problems. This audienceranges from advanced high-school students, who I think will have a ball with it, toundergraduate and graduate students who want some amusing problems to ponder, toprofessors who are looking for a new supply of problems to use in their classes, andfinally to anyone with a desire to learn about physics by doing problems. If you want,you can consider this to be a problem book that also happens to have comprehensivexiiiMORIN: “FM” — 2007/10/9 — 19:08 — page xiii — #13

xivPrefaceintroductions to each topic’s set of problems. With about 250 problems (with includedsolutions) and 350 exercises (without included solutions), in addition to all the examplesin the text, I think you’ll get your money’s worth! But just in case, I threw in 600 figures,50 limericks, nine appearances of the golden ratio, and one cameo of e π .The prerequisites for the book are solid high-school foundations in mechanics(no electricity and magnetism required) and single-variable calculus. There aretwo minor exceptions to this. First, a few sections rely on multivariable calculus, so I have given a review of this in Appendix B. The bulk of it comes inSection 5.3 (which involves the curl), but this section can easily be skipped ona first reading. Other than that, there are just some partial derivatives, dot products, and cross products (all of which are reviewed in Appendix B) sprinkledthroughout the book. Second, a few sections (4.5, 9.2–9.3, and Appendices Dand E) rely on matrices and other elementary topics from linear algebra. But abasic understanding of matrices should suffice here.A brief outline of the book is as follows. Chapter 1 discusses various problemsolving strategies. This material is extremely important, so if you read only onechapter in the book, make it this one. You should keep these strategies on thetip of your brain as you march through the rest of the book. Chapter 2 coversstatics. Most of this will likely be familiar, but you’ll find some fun problems.In Chapter 3, we learn about forces and how to apply F ma. There’s a bit ofmath here needed for solving some simple differential equations. Chapter 4 dealswith oscillations and coupled oscillators. Again, there’s a fair bit of math neededfor solving linear differential equations, but there’s no way to avoid it. Chapter 5deals with conservation of energy and momentum. You’ve probably seen muchof this before, but it has lots of neat problems.In Chapter 6, we introduce the Lagrangian method, which will most likely benew to you. It looks rather formidable at first, but it’s really not all that rough.There are difficult concepts at the heart of the subject, but the nice thing is that thetechnique is easy to apply. The situation here is analogous to taking a derivativein calculus; there are substantive concepts on which the theory rests, but the actof taking a derivative is fairly straightforward.Chapter 7 deals with central forces and planetary motion. Chapter 8 coversthe easier type of angular momentum situations, where the direction of theangular momentum vector is fixed. Chapter 9 covers the more difficult type,where the direction changes. Spinning tops and other perplexing objects fall intothis category. Chapter 10 deals with accelerating reference frames and fictitiousforces.Chapters 11 through 14 cover relativity. Chapter 11 deals with relativistickinematics – abstract particles flying through space and time. Chapter 12 coversrelativistic dynamics – energy, momentum, force, etc. Chapter 13 introduces theimportant concept of “4-vectors.” The material in this chapter could alternativelybe put in the previous two, but for various reasons I thought it best to create aMORIN: “FM” — 2007/10/9 — 19:08 — page xiv — #14

Prefaceseparate chapter for it. Chapter 14 covers a few topics from General Relativity.It’s impossible for one chapter to do this subject justice, of course, so we’ll justlook at some basic (but still very interesting) examples. Finally, the appendicescover various useful, but slightly tangential, topics.Throughout the book, I have included many “Remarks.” These are writtenin a slightly smaller font than the surrounding text. They begin with a smallcapital “Remark” and end with a shamrock ( ). The purpose of these remarks isto say something that needs to be said, without disrupting the overall flow of theargument. In some sense these are “extra” thoughts, although they are invariablyuseful in understanding what is going on. They are usually more informal thanthe rest of the text, and I reserve the right to use them to occasionally babbleabout things that I find interesting, but that you may find tangential. For the mostpart, however, the remarks address issues that arise naturally in the course of thediscussion. I often make use of “Remarks” at the ends of the solutions to problems,where the obvious thing to do is to check limiting cases (this topic is discussed inChapter 1). However, in this case, the remarks are not “extra” thoughts, becausechecking limiting cases of your answer is something you should always do.For your reading pleasure (I hope!), I have included limericks throughout thetext. I suppose that these might be viewed as educational, but they certainly don’trepresent any deep insight I have into the teaching of physics. I have written themfor the sole purpose of lightening things up. Some are funny. Some are stupid.But at least they’re all physically accurate (give or take).As mentioned above, this book contains a huge number of problems. The oneswith included solutions are called “Problems,” and the ones without includedsolutions, which are intended to be used for homework assignments, are called“Exercises.” There is no fundamental difference between these two types, exceptfor the existence of written-up solutions. I have chosen to include the solutionsto the problems for two reasons. First, students invariably want extra practiceproblems, with solutions, to work on. And second, I had a thoroughly enjoyabletime writing them up. But a warning on these problems and exercises: Some areeasy, but many are very difficult. I think you’ll find them quite interesting, butdon’t get discouraged if you have trouble solving them. Some are designed to bebrooded over for hours. Or days, or weeks, or months (as I can attest to!).The problems (and exercises) are marked with a number of stars (actuallyasterisks). Harder problems earn more stars, on a scale from zero to four. Ofcourse, you may disagree with my judgment of difficulty, but I think that anarbitrary weighting scheme is better than none at all. As a rough idea of what Imean by the number of stars, one-star problems are solid problems that requiresome thought, and four-star problems are really, really, really hard. Try a fewand you’ll see what I mean. Even if you understand the material in the textbackwards and forwards, the four-star (and many of the three-star) problems willstill be extremely challenging. But that’s how it should be. My goal was to createan unreachable upper bound on the number (and difficulty) of problems, becauseMORIN: “FM” — 2007/10/9 — 19:08 — page xv — #15xv

xviPrefaceit would be an unfortunate circumstance if you were left twiddling your thumbs,having run out of problems to solve. I hope I have succeeded.For the problems you choose to work on, be careful not to look at the solutiontoo soon. There’s nothing wrong with putting a problem aside for a while andcoming back to it later. Indeed, this is probably the best way to learn things. Ifyou head to the solution at the first sign of not being able to solve a problem,then you have wasted the problem.Remark: This gives me an opportunity for my first remark (and first limerick, too). A fact thatoften gets overlooked is that you need to know more than the correct way(s) to do a problem; youalso need to be familiar with many incorrect ways of doing it. Otherwise, when you come upona new problem, there may be a number of decent-looking approaches to take, and you won’t beable to immediately weed out the poor ones. Struggling a bit with a problem invariably leadsyou down some wrong paths, and this is an essential part of learning. To understand something,you not only have to know what’s right about the right things; you also have to know what’swrong about the wrong things. Learning takes a serious amount of effort, many wrong turns,and a lot of sweat. Alas, there are no shortcuts to understanding physics.The ad said, For one little fee,You can skip all that course-work ennui.So send your tuition,For boundless fruition!Get your mail-order physics degree! Any book that takes ten years to write is bound to contain the (greatly appreciated) input of many people. I am particularly thankful for Howard Georgi’s helpover the years, with his numerous suggestions, ideas for many problems, andphysics sanity checks. I would also like to thank Don Page for his entertainingand meticulous comments and suggestions, and an eye for catching errors in earlier versions. Other friends and colleagues who have helped make this book whatit is (and who have made it all the more fun to write) are John Bechhoefer, WesCampbell, Michelle Cyrier, Alex Dahlen, Gary Feldman, Lukasz Fidkowski,Jason Gallicchio, Doug Goodale, Bertrand Halperin, Matt Headrick, JennyHoffman, Paul Horowitz, Alex Johnson, Yevgeny Kats, Can Kilic, Ben Krefetz,Daniel Larson, Jaime Lush, Rakhi Mahbubani, Chris Montanaro, Theresa Morin,Megha Padi, Dave Patterson, Konstantin Penanen, Courtney Peterson, MalaRadhakrishnan, Esteban Real, Daniel Rosenberg, Wolfgang Rueckner, AqilSajjad, Alexia Schulz, Daniel Sherman, Oleg Shpyrko, David Simmons-Duffin,Steve Simon, Joe Swingle, Edwin Taylor, Sam Williams, Alex Wissner-Gross,and Eric Zaslow. I’m sure that I have forgotten others, especially from the earlieryears where my memory fades, so please accept my apologies.I am also grateful for the highly professional work done by the editorial andproduction group at Cambridge University Press in transforming this into anactual book. It has been a pleasure working with Lindsay Barnes, Simon Capelin,Margaret Patterson, and Dawn Preston.Finally, and perhaps most importantly, I would like to thank all the students(both at Harvard and elsewhere) who provided input during the past decade.MORIN: “FM” — 2007/10/9 — 19:08 — page xvi — #16

PrefaceThe names here are literally too numerous to write down, so let me simply say abig thank you, and that I hope other students will enjoy what you helped create.Despite the painstaking proofreading and all the eyes that have passed overearlier versions, there is at most an exponentially small probability that thebook is error free. So if something looks amiss, please check the webpage(www.cambridge.org/9780521876223) for a list of typos, updates, etc. Andplease let me know if you discover something that isn’t already posted. I’msure that eventually I will post some new problems and supplementary material,so be sure to check the webpage for additions. Information for instructors willalso be available on this site.Happy problem solving – I hope you enjoy the book!MORIN: “FM” — 2007/10/9 — 19:08 — page xvii — #17xvii

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Chapter 1Strategies for solving problemsPhysics involves a great deal of problem solving. Whether you are doingcutting-edge research or reading a book on a well-known subject, you are goingto need to solve some problems. In the latter case (the presently relevant one,given what is in your hand right now), it is fairly safe to say that the true testof understanding something is the ability to solve problems on it. Reading abouta topic is often a necessary step in the learning process, but it is by no meansa sufficient one. The more important step is spending as much time as possiblesolving problems (which is inevitably an active task) beyond the time you spendreading (which is generally a more passive task). I have therefore included a verylarge number of problems/exercises in this book.However, if I’m going to throw all these problems at you, I should at least giveyou some general strategies for solving them. These strategies are the subject ofthe present chapter. They are things you should always keep in the back of yourmind when tackling a problem. Of course, they are generally not sufficient bythemselves; you won’t get too far without understanding the physical conceptsbehind the subject at hand. But when you add these strategies to your physicalunderstanding, they can make your life a lot easier.1.1General strategiesThere are a number of general strategies you should invoke without hesitationwhen solving a problem. They are:1. Draw a diagram, if appropriate.In the diagram, be sure to label clearly all the relevant quantities (forces, lengths,masses, etc.). Diagrams are absolutely critical in certain types of problems. Forexample, in problems involving “free-body” diagrams (discussed in Chapter 3) orrelativistic kinematics (discussed in Chapter 11), drawing a diagram can change ahopelessly complicated problem into a near-trivial one. And even in cases wherediagrams aren’t this crucial, they’re invariably very helpful. A picture is definitelyworth a thousand words (and even a few more, if you label things!).1MORIN: “CHAP01” — 2007/10/9 — 16:06 — page 1 — #1

2Strategies for solving problems2. Write down what you know, and what you are trying to find.In a simple problem, you may just do this in your head without realizing it. But inmore difficult problems, it is very useful to explicitly write things out. For example,if there are three unknowns that you’re trying to find, but you’ve written downonly two facts, then you know there must be another fact you’re missing (assumingthat the problem is in fact solvable), so you can go searching for it. It might be aconservation law, or an F ma equation, etc.3. Solve things symbolically.If you are solving a problem where the given quantities are specified numerically,you should immediately change the numbers to letters and solve the problem in termsof the letters. After you obtain an answer in terms of the letters, you can plug in theactual numerical values to obtain a numerical answer. There are many advantagesto using letters: It’s quicker. It’s much easier to multiply a g by an by writing them down on apiece of paper next to each other, than it is to multiply them together on a calculator.And with the latter strategy, you’d undoubtedly have to pick up your calculator atleast a few times during the course of a problem. You’re less likely to make a mistake. It’s very easy to mistype an 8 for a 9 ina calculator, but you’re probably not going to miswrite a q for a g on a piece ofpaper. But if you do, you’ll quickly realize that it should be a g. You certainlywon’t just give up on the problem and deem it unsolvable because no one gaveyou the value of q! You can do the problem once and for all. If someone comes along and says,oops, the value of is actually 2.4 m instead of 2.3 m, then you won’t have to dothe whole problem again. You can simply plug the new value of into your finalsymbolic answer. You can see the general dependence of your answer on the various given quantities. For example, you can see that it grows with quantities a and b, decreases withc, and doesn’t depend on d. There is much, much more information contained in asymbolic answer than in a numerical one. And besides, symbolic answers nearlyalways look nice and pretty. You can check units and special cases. These checks go hand-in-hand with theprevious “general dependence” advantage. But since they’re so important, we’llpostpone their discussion and devote Sections 1.2 and 1.3 to them.Having said all this, it should be noted that there are occasionally times when thingsget a bit messy when working with letters. For example, solving a system of threeequations in three unknowns might be rather cumbersome unless you plug in theactual numbers. But in the vast majority of problems, it is highly advantageous towork entirely with letters.4. Consider units/dimensions.This is extremely important. See Section 1.2 for a detailed discussion.MORIN: “CHAP01” — 2007/10/9 — 16:06 — page 2 — #2

1.1 General strategies5. Check limiting/special cases.This is also extremely important. See Section 1.3 for a detailed discussion.6. Check order of magnitude if you end up getting a numerical answer.If you end up with an actual numerical answer to a problem, be sure to do a sanity check to see if the number is reasonable. If you’ve calculated the distancealong the ground that a car skids before it comes to rest, and if you’ve gottenan answer of a kilometer or a millimeter, then you know you’ve probably donesomething wrong. Errors of this sort often come from forgetting some powers of10 (say, when converting kilometers to meters) or from multiplying somethinginstead of dividing (although you should be able to catch this by checking yourunits, too).You will inevitably encounter problems, physics ones or otherwise, whereyou don’t end up obtaining a rigorous answer, either because the calculation isintractable, or because you just don’t feel like doing it. But in these cases it’susually still possible to make an educated guess, to the nearest power of 10. Forexample, if you walk past a building and happen to wonder how many bricksare in it, or what the labor cost was in constructing it, then you can probablygive a reasonable answer without doing any severe computations. The physicistEnrico Fermi was known for his ability to estimate things quickly and produceorder-of-magnitude guesses with only minimal calculation. Hence, a problemwhere the goal is to simply obtain the nearest power-of-10 estimate is known as a“Fermi problem.” Of course, sometimes in life you need to know things to betteraccuracy than the nearest power of 10 . . .How Fermi could estimate things!Like the well-known Olympic ten rings,And the one hundred states,And weeks with ten dates,And birds that all fly with one . . . wings.In the following two sections, we’ll discuss the very important strategies ofchecking units and special cases. Then in Section 1.4 we’ll discuss the techniqueof solving problems numerically, which is what you need to do when you end upwith a set of equations you can’t figure out how to solve. Section 1.4 isn’t quiteanalogous to Sections 1.2 and 1.3, in that these first two are relevant to basicallyany problem you’ll ever do, whereas solving equations numerically is somethingyou’ll do only for occasional problems. But it’s nevertheless something that everyphysics student should know.In all three of these sections, we’ll invoke various results derived later in thebook. For the present purposes, the derivations of these results are completelyirrelevant, so don’t worry at all about the physics behind them – there will beMORIN: “CHAP01” — 2007/10/9 — 16:06 — page 3 — #33

4Strategies for solving problemsplenty of opportunity for that later on! The main point here is to learn what to dowith the result of a problem once you’ve obtained it.1.2Units, dimensional analysisThe units, or dimensions, of a quantity are the powers of mass, length, and timeassociated with it. For example, the units of a speed are length per time. Theconsideration of units offers two main benefits. First, looking at units beforeyou start a problem can tell you roughly what the answer has to look like, upto numerical factors. Second, checking units at the end of a calculation (whichis something you should always do) can tell you if your answer has a chance atbeing correct. It won’t tell you that your answer is definitely correct, but it mighttell you that your answer is definitely incorrect. For example, if your goal in aproblem is to find a length, and if you end up with a mass, then you know it’stime to look back over your work.“Your units are wrong!” cried the teacher.“Your church weighs six joules – what a feature!And the people insideAre four hours wide,And eight gauss away from the preacher!”In practice, the second of the above two benefits is what you will generallymake use of. But let’s do a few examples relating to the first benefit, becausethese can be a little more exciting. To solve the three examples below exactly, wewould need to invoke results derived in later chapters. But let’s just see how far wecan get by using only dimensional analysis. We’ll use the “[ ]” notation for units,and we’ll let M stand for mass, L for length, and T for time. For example, we’llwrite a speed as [v] L/T and the gravitational constant as [G] L3 /(MT 2 )(you can figure this out by noting that Gm1 m2 /r 2 has the dimensions of force,which in turn has dimensions ML/T 2 , from F ma). Alternatively, you can justuse the mks units, kg, m, s, instead of M , L, T , respectively.1uExample (Pendulum

1 Strategies for solving problems 1 1.1 General strategies 1 1.2 Units, dimensional analysis 4 1.3 Approximations, limiting cases 7 1.4 Solving differential equations numerically 11 1.5 Problems 14 1.6 Exercises 15 1.7 Solutions 18 2 Statics 22 2.1 Balancing forces 22 2.2 Balancing torques 27 2.3 Problems 30 2.4 Exercises 35 2.5 Solutions 39 3 .

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