Polarization. OpenStax

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1 OpenStax-CNX module: m Polarization OpenStax This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License 4.0 By the end of this section, you will be able to: Abstract Explain the change in intensity as polarized light passes through a polarizing lter Calculate the eect of polarization by reection and Brewster's angle Describe the eect of polarization by scattering Explain the use of polarizing materials in devices such as LCDs Polarizing sunglasses are familiar to most of us. They have a special ability to cut the glare of light reected from water or glass (Figure 1). They have this ability because of a wave characteristic of light called polarization. What is polarization? How is it produced? What are some of its uses? The answers to these questions are related to the wave character of light. Version 1.3: Sep 28, :46 pm

2 OpenStax-CNX module: m Figure 1: These two photographs of a river show the eect of a polarizing lter in reducing glare in light reected from the surface of water. Part (b) of this gure was taken with a polarizing lter and part (a) was not. As a result, the reection of clouds and sky observed in part (a) is not observed in part (b). Polarizing sunglasses are particularly useful on snow and water. (credit a and credit b: modications of work by Amithshs/Wikimedia Commons) 1 Malus's Law Light is one type of electromagnetic (EM) wave. As noted in the previous chapter on Electromagnetic Waves, EM waves are transverse waves consisting of varying electric and magnetic elds that oscillate perpendicular to the direction of propagation (Figure 2). However, in general, there are no specic directions for the oscillations of the electric and magnetic elds; they vibrate in any randomly oriented plane perpendicular to the direction of propagation. Polarization is the attribute that a wave's oscillations do have a denite direction relative to the direction of propagation of the wave. (This is not the same type of polarization as that discussed for the separation of charges.) Waves having such a direction are said to be polarized. For an EM wave, we dene the direction of polarization to be the direction parallel to the electric eld. Thus, we can think of the electric eld arrows as showing the direction of polarization, as in Figure 2.

3 OpenStax-CNX module: m E B Figure 2: An EM wave, such as light, is a transverse wave. The electric and magnetic elds are perpendicular to the direction of propagation. The direction of polarization of the wave is the direction of the electric eld. To examine this further, consider the transverse waves in the ropes shown in Figure 3. The oscillations in one rope are in a vertical plane and are said to be vertically polarized. Those in the other rope are in a horizontal plane and are horizontally polarized. If a vertical slit is placed on the rst rope, the waves pass through. However, a vertical slit blocks the horizontally polarized waves. For EM waves, the direction of the electric eld is analogous to the disturbances on the ropes.

4 OpenStax-CNX module: m Figure 3: The transverse oscillations in one rope (a) are in a vertical plane, and those in the other rope (b) are in a horizontal plane. The rst is said to be vertically polarized, and the other is said to be horizontally polarized. Vertical slits pass vertically polarized waves and block horizontally polarized waves. The Sun and many other light sources produce waves that have the electric elds in random directions (Figure 4(a)). Such light is said to be unpolarized, because it is composed of many waves with all possible directions of polarization. Polaroid materialswhich were invented by the founder of the Polaroid Corporation, Edwin Landact as a polarizing slit for light, allowing only polarization in one direction to pass through. Polarizing lters are composed of long molecules aligned in one direction. If we think of the molecules as many slits, analogous to those for the oscillating ropes, we can understand why only light with a specic polarization can get through. The axis of a polarizing lter is the direction along which the lter passes the electric eld of an EM wave.

5 OpenStax-CNX module: m Figure 4: The slender arrow represents a ray of unpolarized light. The bold arrows represent the direction of polarization of the individual waves composing the ray. (a) If the light is unpolarized, the arrows point in all directions. (b) A polarizing lter has a polarization axis that acts as a slit passing through electric elds parallel to its direction. The direction of polarization of an EM wave is dened to be the direction of its electric eld. Figure 5 shows the eect of two polarizing lters on originally unpolarized light. The rst lter polarizes the light along its axis. When the axes of the rst and second lters are aligned (parallel), then all of the polarized light passed by the rst lter is also passed by the second lter. If the second polarizing lter is rotated, only the component of the light parallel to the second lter's axis is passed. When the axes are perpendicular, no light is passed by the second lter.

6 OpenStax-CNX module: m Figure 5: The eect of rotating two polarizing lters, where the rst polarizes the light. (a) All of the polarized light is passed by the second polarizing lter, because its axis is parallel to the rst. (b) As the second lter is rotated, only part of the light is passed. (c) When the second lter is perpendicular to the rst, no light is passed. (d) In this photograph, a polarizing lter is placed above two others. Its axis is perpendicular to the lter on the right (dark area) and parallel to the lter on the left (lighter area). (credit d: modication of work by P.P. Urone) Only the component of the EM wave parallel to the axis of a lter is passed. Let us call the angle between the direction of polarization and the axis of a lter θ. If the electric eld has an amplitude E, then the transmitted part of the wave has an amplitude E cos θ (Figure 6). Since the intensity of a wave is proportional to its amplitude squared, the intensity I of the transmitted wave is related to the incident wave by note: I = I 0 cos 2 θ (1) where I 0 is the intensity of the polarized wave before passing through the lter. This equation is known as Malus's law.

7 OpenStax-CNX module: m Figure 6: A polarizing lter transmits only the component of the wave parallel to its axis, reducing the intensity of any light not polarized parallel to its axis. note: This Open Source Physics animation 1 helps you visualize the electric eld vectors as light encounters a polarizing lter. You can rotate the lternote that the angle displayed is in radians. You can also rotate the animation for 3D visualization. Example 1 Calculating Intensity Reduction by a Polarizing Filter What angle is needed between the direction of polarized light and the axis of a polarizing lter to reduce its intensity by 90.0%? Strategy When the intensity is reduced by 90.0%, it is 10.0% or times its original value. That is, I = I 0. Using this information, the equation I = I 0 cos 2 θ can be used to solve for the needed angle. Solution Solving the equation I = I 0 cos 2 θ for cos θ and substituting with the relationship between I and I 0 gives Solving for θ yields cos θ = I I0 = = (2) I 0 I 0 1

8 OpenStax-CNX module: m θ = cos = (3) Signicance A fairly large angle between the direction of polarization and the lter axis is needed to reduce the intensity to 10.0% of its original value. This seems reasonable based on experimenting with polarizing lms. It is interesting that at an angle of 45, the intensity is reduced to 50% of its original value. Note that 71.6 is 18.4 from reducing the intensity to zero, and that at an angle of 18.4, the intensity is reduced to 90.0% of its original value, giving evidence of symmetry. note: Exercise 1 (Solution on p. 25.) Check Your Understanding Although we did not specify the direction in Example 1, let's say the polarizing lter was rotated clockwise by 71.6 to reduce the light intensity by 90.0%. What would be the intensity reduction if the polarizing lter were rotated counterclockwise by 71.6? 2 Polarization by Reection By now, you can probably guess that polarizing sunglasses cut the glare in reected light, because that light is polarized. You can check this for yourself by holding polarizing sunglasses in front of you and rotating them while looking at light reected from water or glass. As you rotate the sunglasses, you will notice the light gets bright and dim, but not completely black. This implies the reected light is partially polarized and cannot be completely blocked by a polarizing lter. Figure 7 illustrates what happens when unpolarized light is reected from a surface. Vertically polarized light is preferentially refracted at the surface, so the reected light is left more horizontally polarized. The reasons for this phenomenon are beyond the scope of this text, but a convenient mnemonic for remembering this is to imagine the polarization direction to be like an arrow. Vertical polarization is like an arrow perpendicular to the surface and is more likely to stick and not be reected. Horizontal polarization is like an arrow bouncing on its side and is more likely to be reected. Sunglasses with vertical axes thus block more reected light than unpolarized light from other sources.

9 OpenStax-CNX module: m Figure 7: Polarization by reection. Unpolarized light has equal amounts of vertical and horizontal polarization. After interaction with a surface, the vertical components are preferentially absorbed or refracted, leaving the reected light more horizontally polarized. This is akin to arrows striking on their sides and bouncing o, whereas arrows striking on their tips go into the surface. Since the part of the light that is not reected is refracted, the amount of polarization depends on the indices of refraction of the media involved. It can be shown that reected light is completely polarized at an angle of reection θ b given by note: tan θ b = n 2 n 1 (4) where n 1 is the medium in which the incident and reected light travel and n 2 is the index of refraction of the medium that forms the interface that reects the light. This equation is known as Brewster's law and θ b is known as Brewster's angle, named after the nineteenth-century Scottish physicist who discovered them. note: This Open Source Physics animation 2 shows incident, reected, and refracted light as rays and EM waves. Try rotating the animation for 3D visualization and also change the angle of incidence. Near Brewster's angle, the reected light becomes highly polarized. Example 2 Calculating Polarization by Reection (a) At what angle will light traveling in air be completely polarized horizontally when reected from water? (b) From glass? 2

10 OpenStax-CNX module: m Strategy All we need to solve these problems are the indices of refraction. Air has n 1 = 1.00, water has n 2 = 1.333, and crown glass has n 2 = The equation tan θ b = n2 n 1 can be directly applied to nd θ b in each case. Solution a. Putting the known quantities into the equation gives tan θ b = n 2 n 1 (5) Solving for the angle θ b yields tan θ b = n 2 = = (6) n b. Similarly, for crown glass and air, θ b = tan = (7) Thus, tan θ b = n 2 = = (8) n θ b = tan = (9) Signicance Light reected at these angles could be completely blocked by a good polarizing lter held with its axis vertical. Brewster's angle for water and air are similar to those for glass and air, so that sunglasses are equally eective for light reected from either water or glass under similar circumstances. Light that is not reected is refracted into these media. Therefore, at an incident angle equal to Brewster's angle, the refracted light is slightly polarized vertically. It is not completely polarized vertically, because only a small fraction of the incident light is reected, so a signicant amount of horizontally polarized light is refracted. note: Exercise 2 (Solution on p. 25.) Check Your Understanding What happens at Brewster's angle if the original incident light is already 100% vertically polarized?

11 OpenStax-CNX module: m Atomic Explanation of Polarizing Filters Polarizing lters have a polarization axis that acts as a slit. This slit passes EM waves (often visible light) that have an electric eld parallel to the axis. This is accomplished with long molecules aligned perpendicular to the axis, as shown in Figure 8. Figure 8: Long molecules are aligned perpendicular to the axis of a polarizing lter. In an EM wave, the component of the electric eld perpendicular to these molecules passes through the lter, whereas the component parallel to the molecules is absorbed. Figure 9 illustrates how the component of the electric eld parallel to the long molecules is absorbed. An EM wave is composed of oscillating electric and magnetic elds. The electric eld is strong compared with the magnetic eld and is more eective in exerting force on charges in the molecules. The most aected charged particles are the electrons, since electron masses are small. If an electron is forced to oscillate, it can absorb energy from the EM wave. This reduces the eld in the wave and, hence, reduces its intensity. In long molecules, electrons can more easily oscillate parallel to the molecule than in the perpendicular direction.

12 OpenStax-CNX module: m The electrons are bound to the molecule and are more restricted in their movement perpendicular to the molecule. Thus, the electrons can absorb EM waves that have a component of their electric eld parallel to the molecule. The electrons are much less responsive to electric elds perpendicular to the molecule and allow these elds to pass. Thus, the axis of the polarizing lter is perpendicular to the length of the molecule. Figure 9: Diagram of an electron in a long molecule oscillating parallel to the molecule. The oscillation of the electron absorbs energy and reduces the intensity of the component of the EM wave that is parallel to the molecule. 4 Polarization by Scattering If you hold your polarizing sunglasses in front of you and rotate them while looking at blue sky, you will see the sky get bright and dim. This is a clear indication that light scattered by air is partially polarized. Figure 10 helps illustrate how this happens. Since light is a transverse EM wave, it vibrates the electrons of air molecules perpendicular to the direction that it is traveling. The electrons then radiate like small antennae. Since they are oscillating perpendicular to the direction of the light ray, they produce EM radiation that is polarized perpendicular to the direction of the ray. When viewing the light along a line perpendicular to the original ray, as in the gure, there can be no polarization in the scattered light parallel to the original ray, because that would require the original ray to be a longitudinal wave. Along other directions, a component of the other polarization can be projected along the line of sight, and the scattered light is only partially polarized. Furthermore, multiple scattering can bring light to your eyes from other directions and can contain dierent polarizations.

13 OpenStax-CNX module: m Figure 10: Polarization by scattering. Unpolarized light scattering from air molecules shakes their electrons perpendicular to the direction of the original ray. The scattered light therefore has a polarization perpendicular to the original direction and none parallel to the original direction. Photographs of the sky can be darkened by polarizing lters, a trick used by many photographers to make clouds brighter by contrast. Scattering from other particles, such as smoke or dust, can also polarize light. Detecting polarization in scattered EM waves can be a useful analytical tool in determining the scattering source. A range of optical eects are used in sunglasses. Besides being polarizing, sunglasses may have colored pigments embedded in them, whereas others use either a nonreective or reective coating. A recent development is photochromic lenses, which darken in the sunlight and become clear indoors. Photochromic lenses are embedded with organic microcrystalline molecules that change their properties when exposed to UV in sunlight, but become clear in articial lighting with no UV. 5 Liquid Crystals and Other Polarization Eects in Materials Although you are undoubtedly aware of liquid crystal displays (LCDs) found in watches, calculators, computer screens, cellphones, at screen televisions, and many other places, you may not be aware that they are based on polarization. Liquid crystals are so named because their molecules can be aligned even though they are in a liquid. Liquid crystals have the property that they can rotate the polarization of light passing through them by 90. Furthermore, this property can be turned o by the application of a voltage, as illustrated in Figure 11. It is possible to manipulate this characteristic quickly and in small, well-dened regions to create the contrast patterns we see in so many LCD devices.

14 OpenStax-CNX module: m In at screen LCD televisions, a large light is generated at the back of the TV. The light travels to the front screen through millions of tiny units called pixels (picture elements). One of these is shown in Figure 11(a) and (b). Each unit has three cells, with red, blue, or green lters, each controlled independently. When the voltage across a liquid crystal is switched o, the liquid crystal passes the light through the particular lter. We can vary the picture contrast by varying the strength of the voltage applied to the liquid crystal. Figure 11: (a) Polarized light is rotated 90 by a liquid crystal and then passed by a polarizing lter that has its axis perpendicular to the direction of the original polarization. (b) When a voltage is applied to the liquid crystal, the polarized light is not rotated and is blocked by the lter, making the region dark in comparison with its surroundings. (c) LCDs can be made color specic, small, and fast enough to use in laptop computers and TVs. Many crystals and solutions rotate the plane of polarization of light passing through them. Such substances are said to be optically active. Examples include sugar water, insulin, and collagen (Figure 12). In addition to depending on the type of substance, the amount and direction of rotation depend on several other factors. Among these is the concentration of the substance, the distance the light travels through it, and the wavelength of light. Optical activity is due to the asymmetrical shape of molecules in the substance, such as being helical. Measurements of the rotation of polarized light passing through substances can thus be used to measure concentrations, a standard technique for sugars. It can also give information on the shapes of molecules, such as proteins, and factors that aect their shapes, such as temperature and ph.

15 OpenStax-CNX module: m Figure 12: Optical activity is the ability of some substances to rotate the plane of polarization of light passing through them. The rotation is detected with a polarizing lter or analyzer. Glass and plastic become optically active when stressed: the greater the stress, the greater the eect. Optical stress analysis on complicated shapes can be performed by making plastic models of them and observing them through crossed lters, as seen in Figure 13. It is apparent that the eect depends on wavelength as well as stress. The wavelength dependence is sometimes also used for artistic purposes.

16 OpenStax-CNX module: m Figure 13: Optical stress analysis of a plastic lens placed between crossed polarizers. (credit: Infopro/Wikimedia Commons) Another interesting phenomenon associated with polarized light is the ability of some crystals to split an unpolarized beam of light into two polarized beams. This occurs because the crystal has one value for the

17 OpenStax-CNX module: m index of refraction of polarized light but a dierent value for the index of refraction of light polarized in the perpendicular direction, so that each component has its own angle of refraction. Such crystals are said to be birefringent, and, when aligned properly, two perpendicularly polarized beams will emerge from the crystal (Figure 14). Birefringent crystals can be used to produce polarized beams from unpolarized light. Some birefringent materials preferentially absorb one of the polarizations. These materials are called dichroic and can produce polarization by this preferential absorption. This is fundamentally how polarizing lters and other polarizers work. Figure 14: Birefringent materials, such as the common mineral calcite, split unpolarized beams of light into two with two dierent values of index of refraction. 6 Summary ˆ Polarization is the attribute that wave oscillations have a denite direction relative to the direction of propagation of the wave. The direction of polarization is dened to be the direction parallel to the electric eld of the EM wave. ˆ Unpolarized light is composed of many rays having random polarization directions. ˆ Unpolarized light can be polarized by passing it through a polarizing lter or other polarizing material. The process of polarizing light decreases its intensity by a factor of 2. ˆ The intensity, I, of polarized light after passing through a polarizing lter is I = I 0 cos 2 θ, where I 0 is the incident intensity and θ is the angle between the direction of polarization and the axis of the lter. ˆ Polarization is also produced by reection. ˆ Brewster's law states that reected light is completely polarized at the angle of reection θ b, known as Brewster's angle. ˆ Polarization can also be produced by scattering. ˆ Several types of optically active substances rotate the direction of polarization of light passing through them.

18 OpenStax-CNX module: m Key Equations Speed of light Index of refraction Law of reection c = m/s m/s n = c v θ r = θ i Law of refraction (Snell's law) n 1 sin θ 1 = ( n 2 sin θ ) 2 Critical angle θ c = sin 1 n 2 n 1 for n 1 > n 2 Malus's law Brewster's law I = I 0 cos 2 θ tan θ b = n2 n 1 Table 1 8 Conceptual Questions Exercise 3 (Solution on p. 25.) Can a sound wave in air be polarized? Explain. Exercise 4 No light passes through two perfect polarizing lters with perpendicular axes. However, if a third polarizing lter is placed between the original two, some light can pass. Why is this? Under what circumstances does most of the light pass? Exercise 5 (Solution on p. 25.) Explain what happens to the energy carried by light that it is dimmed by passing it through two crossed polarizing lters. Exercise 6 When particles scattering light are much smaller than its wavelength, the amount of scattering is proportional to 1 λ. Does this mean there is more scattering for small λ than large λ? How does this relate to the fact that the sky is blue? Exercise 7 (Solution on p. 25.) Using the information given in the preceding question, explain why sunsets are red. Exercise 8 When light is reected at Brewster's angle from a smooth surface, it is 100% polarized parallel to the surface. Part of the light will be refracted into the surface. Describe how you would do an experiment to determine the polarization of the refracted light. What direction would you expect the polarization to have and would you expect it to be 100%? Exercise 9 (Solution on p. 25.) If you lie on a beach looking at the water with your head tipped slightly sideways, your polarized sunglasses do not work very well. Why not? 9 Problems Exercise 10 What angle is needed between the direction of polarized light and the axis of a polarizing lter to cut its intensity in half?

19 OpenStax-CNX module: m Exercise 11 (Solution on p. 25.) The angle between the axes of two polarizing lters is By how much does the second lter reduce the intensity of the light coming through the rst? Exercise 12 Two polarizing sheets P 1 and P 2 are placed together with their transmission axes oriented at an angle θ to each other. What is θ when only 25% of the maximum transmitted light intensity passes through them? Exercise 13 (Solution on p. 25.) Suppose that in the preceding problem the light incident on P 1 is unpolarized. At the determined value of θ, what fraction of the incident light passes through the combination? Exercise 14 If you have completely polarized light of intensity 150 W/m 2, what will its intensity be after passing through a polarizing lter with its axis at an 89.0 angle to the light's polarization direction? Exercise 15 (Solution on p. 25.) What angle would the axis of a polarizing lter need to make with the direction of polarized light of intensity 1.00 kw/m 2 to reduce the intensity to 10.0 W/m 2? Exercise 16 At the end of Example 1, it was stated that the intensity of polarized light is reduced to 90.0% of its original value by passing through a polarizing lter with its axis at an angle of 18.4 to the direction of polarization. Verify this statement. Exercise 17 (Solution on p. 25.) Show that if you have three polarizing lters, with the second at an angle of 45.0 to the rst and the third at an angle of 90.0 to the rst, the intensity of light passed by the rst will be reduced to 25.0% of its value. (This is in contrast to having only the rst and third, which reduces the intensity to zero, so that placing the second between them increases the intensity of the transmitted light.) Exercise 18 Three polarizing sheets are placed together such that the transmission axis of the second sheet is oriented at 25.0 to the axis of the rst, whereas the transmission axis of the third sheet is oriented at 40.0 (in the same sense) to the axis of the rst. What fraction of the intensity of an incident unpolarized beam is transmitted by the combination? Exercise 19 (Solution on p. 25.) In order to rotate the polarization axis of a beam of linearly polarized light by 90.0, a student places sheets P 1 and P 2 with their transmission axes at 45.0 and 90.0, respectively, to the beam's axis of polarization. (a) What fraction of the incident light passes through P 1 and (b) through the combination? (c) Repeat your calculations for part (b) for transmission-axis angles of 30.0 and 90.0, respectively. Exercise 20 It is found that when light traveling in water falls on a plastic block, Brewster's angle is What is the refractive index of the plastic? Exercise 21 (Solution on p. 25.) At what angle will light reected from diamond be completely polarized? Exercise 22 What is Brewster's angle for light traveling in water that is reected from crown glass? Exercise 23 (Solution on p. 25.) A scuba diver sees light reected from the water's surface. At what angle will this light be completely polarized?

20 OpenStax-CNX module: m Additional Problems Exercise 24 From his measurements, Roemer estimated that it took 22 min for light to travel a distance equal to the diameter of Earth's orbit around the Sun. (a) Use this estimate along with the known diameter of Earth's orbit to obtain a rough value of the speed of light. (b) Light actually takes 16.5 min to travel this distance. Use this time to calculate the speed of light. Exercise 25 (Solution on p. 25.) Cornu performed Fizeau's measurement of the speed of light using a wheel of diameter 4.00 cm that contained 180 teeth. The distance from the wheel to the mirror was 22.9 km. Assuming he measured the speed of light accurately, what was the angular velocity of the wheel? Exercise 26 Suppose you have an unknown clear substance immersed in water, and you wish to identify it by nding its index of refraction. You arrange to have a beam of light enter it at an angle of 45.0, and you observe the angle of refraction to be What is the index of refraction of the substance and its likely identity? Exercise 27 (Solution on p. 25.) Shown below is a ray of light going from air through crown glass into water, such as going into a sh tank. Calculate the amount the ray is displaced by the glass ( x), given that the incident angle is 40.0 and the glass is 1.00 cm thick.

21 OpenStax-CNX module: m Exercise 28 Considering the previous problem, show that θ 3 is the same as it would be if the second medium were not present. Exercise 29 (Solution on p. 25.) At what angle is light inside crown glass completely polarized when reected from water, as in a sh tank? Exercise 30 Light reected at 55.6 from a window is completely polarized. What is the window's index of refraction and the likely substance of which it is made? Exercise 31 (Solution on p. 25.) (a) Light reected at 62.5 from a gemstone in a ring is completely polarized. Can the gem be a diamond? (b) At what angle would the light be completely polarized if the gem was in water? Exercise 32 If θ b is Brewster's angle for light reected from the top of an interface between two substances,

22 OpenStax-CNX module: m and θ b is Brewster's angle for light reected from below, prove that θ b + θ b = Exercise 33 (Solution on p. 25.) Unreasonable results Suppose light travels from water to another substance, with an angle of incidence of 10.0 and an angle of refraction of (a) What is the index of refraction of the other substance? (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent? Exercise 34 Unreasonable results Light traveling from water to a gemstone strikes the surface at an angle of 80.0 and has an angle of refraction of (a) What is the speed of light in the gemstone? (b) What is unreasonable about this result? (c) Which assumptions are unreasonable or inconsistent? Exercise 35 (Solution on p. 25.) If a polarizing lter reduces the intensity of polarized light to 50.0% of its original value, by how much are the electric and magnetic elds reduced? Exercise 36 Suppose you put on two pairs of polarizing sunglasses with their axes at an angle of How much longer will it take the light to deposit a given amount of energy in your eye compared with a single pair of sunglasses? Assume the lenses are clear except for their polarizing characteristics. Exercise 37 (Solution on p. 25.) (a) On a day when the intensity of sunlight is 1.00 kw/m 2, a circular lens m in diameter focuses light onto water in a black beaker. Two polarizing sheets of plastic are placed in front of the lens with their axes at an angle of Assuming the sunlight is unpolarized and the polarizers are 100% ecient, what is the initial rate of heating of the water in C/s, assuming it is 80.0% absorbed? The aluminum beaker has a mass of 30.0 grams and contains 250 grams of water. (b) Do the polarizing lters get hot? Explain. 11 Challenge Problems Exercise 38 Light shows staged with lasers use moving mirrors to swing beams and create colorful eects. Show that a light ray reected from a mirror changes direction by 2θ when the mirror is rotated by an angle θ. Exercise 39 (Solution on p. 25.) Consider sunlight entering Earth's atmosphere at sunrise and sunsetthat is, at a 90.0 incident angle. Taking the boundary between nearly empty space and the atmosphere to be sudden, calculate the angle of refraction for sunlight. This lengthens the time the Sun appears to be above the horizon, both at sunrise and sunset. Now construct a problem in which you determine the angle of refraction for dierent models of the atmosphere, such as various layers of varying density. Your instructor may wish to guide you on the level of complexity to consider and on how the index of refraction varies with air density. Exercise 40 A light ray entering an optical ber surrounded by air is rst refracted and then reected as shown below. Show that if the ber is made from crown glass, any incident ray will be totally internally reected.

23 OpenStax-CNX module: m Exercise 41 (Solution on p. 25.) A light ray falls on the left face of a prism (see below) at the angle of incidence θ for which the emerging beam has an angle of refraction θ at the right face. Show that the index of refraction n of the glass prism is given by n = sin 1 2 (α+ϕ) sin 1 2 ϕ where ϕ is the vertex angle of the prism and α is the angle through which the beam has been deviated. If α = 37.0 and the base angles of the prism are each 50.0, what is n? Exercise 42 If the apex angle ϕ in the previous problem is 20.0 and n = 1.50, what is the value of α? Exercise 43 (Solution on p. 25.) The light incident on polarizing sheet P 1 is linearly polarized at an angle of 30.0 with respect to the transmission axis of P 1. Sheet P 2 is placed so that its axis is parallel to the polarization axis of

24 OpenStax-CNX module: m the incident light, that is, also at 30.0 with respect to P 1. (a) What fraction of the incident light passes through P 1? (b) What fraction of the incident light is passed by the combination? (c) By rotating P 2, a maximum in transmitted intensity is obtained. What is the ratio of this maximum intensity to the intensity of transmitted light when P 2 is at 30.0 with respect to P 1? Exercise 44 Prove that if I is the intensity of light transmitted by two polarizing lters with axes at an angle θ and I is the intensity when the axes are at an angle 90.0 θ, then I + I = I 0, the original intensity. (Hint: Use the trigonometric identities cos 90.0 θ = sin θ and cos 2 θ + sin 2 θ = 1.

25 OpenStax-CNX module: m Solutions to Exercises in this Module Solution to Exercise (p. 8) also 90.0% Solution to Exercise (p. 10) There will be only refraction but no reection. Solution to Exercise (p. 18) No. Sound waves are not transverse waves. Solution to Exercise (p. 18) Energy is absorbed into the lters. Solution to Exercise (p. 18) Sunsets are viewed with light traveling straight from the Sun toward us. When blue light is scattered out of this path, the remaining red light dominates the overall appearance of the setting Sun. Solution to Exercise (p. 18) The axis of polarization for the sunglasses has been rotated 90. Solution to Exercise (p. 19) Solution to Exercise (p. 19) or 1/8 Solution to Exercise (p. 19) 84.3 Solution to Exercise (p. 19) I 0 Solution to Exercise (p. 19) a ; b ; c Solution to Exercise (p. 19) Solution to Exercise (p. 19) 53.1 Solution to Exercise (p. 20) 114 radian/s Solution to Exercise (p. 20) 3.72 mm Solution to Exercise (p. 21) 41.2 Solution to Exercise (p. 21) a The gem is not a diamond (it is zircon). b Solution to Exercise (p. 22) a ; b. We cannot have n < 1.00, since this would imply a speed greater than c. c. The refracted angle is too big relative to the angle of incidence. Solution to Exercise (p. 22) B 1 Solution to Exercise (p. 22) a C/s; b. yes Solution to Exercise (p. 22) First part: The remainder depends on the complexity of the solution the reader constructs. Solution to Exercise (p. 23) proof; 1.33 Solution to Exercise (p. 23) a ; b ; c. 1.33

26 OpenStax-CNX module: m Glossary Denition 1: birefringent refers to crystals that split an unpolarized beam of light into two beams Denition 2: Brewster's angle angle of incidence at which the reected light is completely polarized Denition 3: Brewster's law tan θ b = n2 n 1, where n 1 is the medium in which the incident and reected light travel and n 2 is the index of refraction of the medium that forms the interface that reects the light Denition 4: direction of polarization direction parallel to the electric eld for EM waves Denition 5: horizontally polarized oscillations are in a horizontal plane Denition 6: Malus's law where I 0 is the intensity of the polarized wave before passing through the lter Denition 7: optically active substances that rotate the plane of polarization of light passing through them Denition 8: polarization attribute that wave oscillations have a denite direction relative to the direction of propagation of the wave Denition 9: polarized refers to waves having the electric and magnetic eld oscillations in a denite direction Denition 10: unpolarized refers to waves that are randomly polarized Denition 11: vertically polarized oscillations are in a vertical plane