The solid lines are physicallypossible paths for light raystraveling from A to B and fromA to C. They obey the principleof least time. The dashed linesdo not obey the principle ofleast time, and are not physicallypossible.s / Paths AQB and APB aretwo conceivable paths that a raycould follow to get from A to Bwith one reflection, but only AQBis physically possible. We wishto prove that the path AQB, withequal angles of incidence andreflection, is shorter than anyother path, such as APB. Thetrick is to construct a third point,C, lying as far below the surfaceas B lies above it. Then pathAQC is a straight line whoselength is the same as AQB’s, andpath APC has the same length aspath APB. Since AQC is straight,it must be shorter than any otherpath such as APC that connectsA and C, and therefore AQB mustbe shorter than any path such asAPB.happen to the velocity components of a light ray that hits a corner, asshown in the figure, and undergoes two reflections?C Three pieces of sheet metal arranged perpendicularly as shown inthe figure form what is known as a radar corner. Let’s assume that theradar corner is large compared to the wavelength of the radar waves, sothat the ray model makes sense. If the radar corner is bathed in radarrays, at least some of them will undergo three reflections. Making a furthergeneralization of your reasoning from the two preceding discussionquestions, what will happen to the three velocity components of such aray? What would the radar corner be useful for?7.3 ⋆ The Principle of Least Time for ReflectionThere is another way of stating the rules of reflection that is verysimple and beautiful, and turns out to have deep consequences andapply much more broadly, not just to reflection. It is called theprinciple of least time, or Fermat’s principle.Let’s start with the motion of light that is not interacting withmatter at all. In a vacuum, a light ray moves in a straight line. Thiscan be rephrased as follows: of all the conceivable paths light couldfollow from P to Q, the only one that is physically possible is thepath that takes the least time.What about reflection? If light is going to go from one point toanother, being reflected on the way, the quickest path is indeed theone with equal angles of incidence and reflection. If the starting andending points are equally far from the reflecting surface, r, it’s nothard to convince yourself that this is true, just based on symmetry.There is also a tricky and simple proof, shown in figure s, for themore general case where the points are at different distances fromthe surface.Not only does the principle of least time work for light in avacuum and light undergoing reflection, we will also see in a laterchapter that it works for the bending of light when it passes fromone medium into another.Although it is beautiful that the entire ray model of light canbe reduced to one simple rule, the principle of least time, it mayseem a little spooky to speak as if the ray of light is intelligent,and has carefully planned ahead to find the shortest route to itsdestination. How does it know in advance where it’s going? Whatif we moved the mirror while the light was en route, so conditionsalong its planned path were not what it “expected?” The answer isthat the principle of least time is really an approximate shortcut forfinding certain results of the wave model of light.There are a couple of subtle points about the principle of leasttime. First, the path does not have to be the quickest of all possiblepaths; it only needs to be quicker than any path that differs148 Chapter 7 The Ray Model of Light
infinitesimally from it. In figure s, for instance, light could get fromA to B either by the reflected path AQB or simply by going straightfrom A to B. Although AQB is not the shortest possible path, itcannot be shortened by changing it infinitesimally, e.g., by movingQ a little to the right or left. On the other hand, path APB is physicallyimpossible, because it is possible to improve on it by movingpoint P infinitesimally to the right.It’s not quite right to call this the principle of least time. In figuret, for example, the four physically possible paths by which a raycan return to the center consist of two shortest-time paths and twolongest-time paths. Strictly speaking, we should refer to the principleof least or greatest time, but most physicists omit the niceties,and assume that other physicists understand that both maxima andminima are possible.7.4 Images by ReflectionInfants are always fascinated by the antics of the Baby in the Mirror.Now if you want to know something about mirror images that mostpeople don’t understand, try this. First bring this page closer wandcloser to your eyes, until you can no longer focus on it withoutstraining. Then go in the bathroom and see how close you canget your face to the surface of the mirror before you can no longereasily focus on the image of your own eyes. You will find thatthe shortest comfortable eye-mirror distance is much less than theshortest comfortable eye-paper distance. This demonstrates thatthe image of your face in the mirror acts as if it had depth andexisted in the space behind the mirror. If the image was like a flatpicture in a book, then you wouldn’t be able to focus on it fromsuch a short distance.In this chapter we will study the images formed by flat andcurved mirrors on a qualitative, conceptual basis. Although thistype of image is not as commonly encountered in everyday life asimages formed by lenses, images formed by reflection are simpler tounderstand.t / Light is emitted at the centerof an elliptical mirror. There arefour physically possible paths bywhich a ray can be reflected andreturn to the center.A virtual imageWe can understand a mirror image using a ray diagram. Figureu shows several light rays, 1, that originated by diffuse reflection atthe person’s nose. They bounce off the mirror, producing new rays,2. To anyone whose eye is in the right position to get one of theserays, they appear to have come from a behind the mirror, 3, wherethey would have originated from a single point. This point is wherethe tip of the image-person’s nose appears to be. A similar analysisapplies to every other point on the person’s face, so it looks asthough there was an entire face behind the mirror. The customaryway of describing the situation requires some explanation:u / An image formed by amirror.Section 7.4 Images by Reflection 149
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ContentsMomentum compared to kineti
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Chapter 1Conservation of Mass andEn
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1.2 Conservation of MassWe intuitiv
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masses on the spring, and they both
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A common source of confusion is the
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Discussion questionA Each of the fo
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l / Galileo Galilei was the first p
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that this wasn’t really an argume
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the girl on the left goes up a cert
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1. kinetic energy2. gravitational e
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In fact, your body uses up even mor
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kinetic energy is twice as much. Bu
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ather than flying off straight. New
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of mass?Actually they’re not even
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ecause the square of the speed of l
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ProblemsKey√∫⋆A computerized
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13 How high above the surface of th
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Chapter 2Conservation ofMomentumFan
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win the Martian version of the Nobe
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a / How can we prove that this coll
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all.This is exactly like the rules
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Unequal masses example 4⊲ Suppose
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ForceDefinition of forceWhen moment
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ent relationship:(fingers on scale)
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pressed in modern units). If the ea
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p / A bowling ball is in the back o
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Kepler’s law of periodsLet T , ca
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2.5 WorkImagine a black box 8 , con
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A tornado touches down in Spring Hi
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pensated for by an overall increase
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Kepler’s equal-area law example 4
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Torque distinguished from forceOf c
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Chapter 4RelativityComplaining abou
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motion of the apparatus. For instan
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fore Einstein. In fact, George Fitz
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We are used to thinking of time as
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j / In the garage’s frame of refe
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is now sufficiently advanced to all
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astronauts had twin siblings back o
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The derivation of the correct relat
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efore the collision0 1.60.9 0.7afte
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e the same as they always were. The
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(b) Show that your result is approx
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Chapter 5ElectricityWhere the teles
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