# Lecture 14 Images Chapter 34

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1 Lecture 4 Images Chapter 34

2 Preliminary topics before mirrors and lenses Law of Reflection Dispersion Snell s Law Brewsters Angle

3 Law of Reflection Dispersion Snell s Law Brewsters Angle

4 Geometrical Optics:Study of reflection and refraction of light from surfaces The ray approximation states that light travels in straight lines until it is reflected or refracted and then travels in straight lines again. The wavelength of light must be small compared to the size of the objects or else diffractive effects occur.

5 Law of Reflection! I =! R Mirror B! r! i A

6 Drawing Normals

7 Fermat s Principle Using Fermat s Principle you can prove the Reflection law. It states that the path taken by light when traveling from one point to another is the path that takes the shortest time compared to nearby paths.

8 Two light rays and 2 taking different paths between points A and B and reflecting off a vertical mirror B Plane Mirror 2 A Use calculus - method of minimization

9 t = ( h 2 C + y 2 + h (w! y) 2 ) dt dy = 2y h 2 + y +!2(w! y) 2 h (w! y) 2 ) = 0 y h 2 + y = (w! y) 2 h (w! y) 2 ) Write down time as a function of y and set the derivative to 0. sin" I = sin" R! I =! R

10 Law of Refraction: Snells Law n sin! = n 2 sin! 2 How do we prove it? n n 2 v sin! = v 2 sin! 2 Air.0 Glass.33

11 t = ( v h 2 + y 2 + v 2 h (w! y) 2 ) dt dy = 0 v sin" I = v 2 sin" R n sin! I = n 2 sin! R

12 JAVA APPLET Show Fermat s principle simulator

13 Dispersion What allows you to see various colors when white light passes through a prism

14 How does a Rainbow work?

15 Dispersion: Different wavelengths have different velocities and therefore different indices of refraction. This leads to different refractive angles for different wavelengths. Thus the light is dispersed. The frequency dose not change when n changes. v = f!! changes when medium changes f does not change when medium changes

16 Why is light totally reflected inside a fiber optics cable? Internal reflection n sin! = n 2 sin! 2 (.33)sin! = (.00)sin90 =.00 When! " sin #.33 " deg light won't get out of the material

17 Fiber Cable Same here

18 Corner Reflector?

19 Show Total Internal reflection simulator Halliday, Resnick, Walker: Fundamentals of Physics, 7th Edition - Student Companion Site

20 What causes a Mirage sky eye Index of refraction Hot road causes gradient in the index of refraction that increases as you increase the distance from the road

21 Inverse Mirage Bend

22 Snells Law Example 47. In the figure, a 2.00-m-long vertical pole extends from the bottom of a swimming pool to a point 50.0 cm above the water. What is the length of the shadow of the pole on the level bottom of the pool? Consider a ray that grazes the top of the pole, as shown in the diagram below. Here! = 35 o, l = 0.50 m, and l 2 =.50 m. The length of the shadow is x + L. x is given by x = l tan! = (0.50m)tan35 o = 0.35 m. air! l L is given by water! 2 L=l 2 tan! 2 l 2 Use Snells Law to find! 2 shadow L x

23 Calculation of L According to the law of refraction, n 2 sin! 2 = n sin!. We take n = and n 2 =.33 ( & # o ' sin( ' sin 35 2 = sin \$ = sin = n! \$ 2.33! % " & % # " o L is given by L = l 2 tan! 2 = (.50m) tan o = 0.72m. air water! l The length of the shadow is L+x. L+x = 0.35m m =.07 m.! 2 shadow l 2 L x

24 Polarization by Reflection Brewsters Law (.)sin! B = nsin! r! B +! r = 90 we get 00% polarized reflected wave sin! B = nsin(90 "! B ) = ncos! B! B = tan " n Brewsters Law

25 Mirrors and Lenses Plane Mirrors Where is the image formed

26 Plane mirrors Real side Angle of incidence Normal Virtual side Virtual image Angle of reflection eye i = - p Object distance = - image distance Image size = Object size

27 Problem: Two plane mirrors make an angle of 90 o. How many images are there for an object placed between them? mirror eye 2 object mirror 3

28 Problem: Two plan mirrors make an angle of 60 o. Find all images for a point object on the bisector. 2 mirror 4 eye object mirror 5,6 3

29 Using the Law of Reflection to make a bank shot Assuming no spin Assuming an elastic collision No cushion deformation d d pocket

30 i = - p magnification = What happens if we bend the mirror? Concave mirror. Image gets magnified. Field of view is diminished Convex mirror. Image is reduced. Field of view increased.

31 Rules for drawing images for mirrors Initial parallel ray reflects through focal point. Ray that passes in initially through focal point reflects parallel from mirror Ray reflects from C the radius of curvature of mirror reflects along itself. Ray that reflects from mirror at little point c is reflected symmetrically p + i = f m =!i p

32

33 Concept Simulator/Illustrations Halliday, Resnick, Walker: Fundamentals of Physics, 7th Edition - Student Companion Site

34 Spherical refracting surfaces Using Snell s Law and assuming small Angles between the rays with the central axis, we get the following formula: n p + n 2 i = n 2! n r

35 Apply this equation to Thin Lenses where the thickness is small compared to object distance, image distance, and radius of curvature. Neglect thickness. Converging lens Diverging lens

36 Thin Lens Equation Lensmaker Equation f = p + i f = (n!)( r! r 2 ) Lateral Magnification for a Lens m =! i p What is the sign convention?

37 Sign Convention Light Virtual side - V r r 2 Real side - R p i Real object - distance p is pos on V side (Incident rays are diverging) Radius of curvature is pos on R side. Real image - distance is pos on R side. Virtual object - distance is neg on R side. Incident rays are converging) Radius of curvature is neg on the V side. Virtual image- distance is neg on the V side.

38 Rules for drawing rays to locate images from a lens A ray initially parallel to the central axis will pass through the focal point. A ray that initially passes through the focal point will emerge from the lens parallel to the central axis. A ray that is directed towards the center of the lens will go straight through the lens undeflected.

39 Example of drawing images

40 Example 24(b). Given a lens with a focal length f = 5 cm and object distance p = +0 cm, find the following: i and m. Is the image real or virtual? Upright or inverted? Draw 3 rays. Virtual side Real side.. F F 2 p = i f! p i = 5! 0 = + 0 i = +0 cm m = y! y = " i p m =! 0 0 =! Image is real, inverted.

41 24(e). Given a lens with the properties (lengths in cm) r = +30, r 2 = -30, p = +0, and n =.5, find the following: f, i and m. Is the image real or virtual? Upright or inverted? Draw 3 rays. Virtual side Real side.. r 2 p F F 2 r f = & # ( n ' ) \$ '! % r r2 " = i f! p m = y! y = " i p f = & \$ % (.5 ' ) 30 ' ' 30 #! " = 30 = i 30! 0 =! 5 m =!!5 0 = +.5 f = 30cm i =! 5cm Image is virtual, upright.

42 27. A converging lens with a focal length of +20 cm is located 0 cm to the left of a diverging lens having a focal length of -5 cm. If an object is located 40 cm to the left of the converging lens, locate and describe completely the final image formed by the diverging lens. Treat each lens Separately. Lens Lens f f 2 f f

43 Lens Lens f f 2 f f Ignoring the diverging lens (lens 2), the image formed by the converging lens (lens ) is located at a distance i = f! p = 20cm! 40cm. i = 40cm Since m = -i /p = - 40/40= -, the image is inverted This image now serves as a virtual object for lens 2, with p 2 = - (40 cm - 0 cm) = - 30 cm.

44 Lens Lens f f 2 f f i 2 = f 2! p 2 =!5cm!!30cm i 2 =!30cm. Thus, the image formed by lens 2 is located 30 cm to the left of lens 2. It is virtual (since i 2 < 0). The magnification is m = (-i /p ) x (-i 2 /p 2 ) = (-40/40)x(30/-30) =+, so the image has the same size orientation as the object.

45 Optical Instruments Magnifying lens Compound microscope Refracting telescope

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