Physics 6C. Geometric Optics Mirrors and Thin Lenses

Transcription

1 Physics 6C Geometric Optics Mirrors and Thin Lenses

2 We have already learned the basics of Reflection and Refraction. Reflection: angle of incidence = angle of reflection Refraction: light bends toward the normal according to Snell s Law Now we apply those concepts to some simple types of mirrors and lenses.

3 We have already learned the basics of Reflection and Refraction: Reflection - angle of incidence = angle of reflection Refraction - light bends toward the normal according to Snell s Law Now we apply those concepts to some simple types of mirrors and lenses. Flat Mirror This is the simplest mirror a flat reflecting surface. The light rays bounce off and you see an image that seems to be behind the mirror. This is called a VIRTUAL IMAGE because the light rays do not actually travel behind the mirror. The image will appear reversed, but will be the same size and the same distance from the mirror. A typical light ray entering the eye of the viewer is shown. The object distance is labeled S and the image distance is labeled S. Real Object Virtual Image S S

4 Spherical Mirrors For curved mirrors we will assume that the shape is spherical (think of a big shiny ball, and slice off any piece of that there s your spherical mirror). This will make our math relatively simple, with only a couple of formulas. The hard part will be to get the negative signs correct. The radius of curvature describes the shape of the mirror. This is the same as the radius of the big shiny ball that the mirror was cut from. We will have two types of mirrors, depending on which direction they curve: CONCAVE mirrors curve toward you, and have POSITIVE R (like the inside of the sphere). CONVEX mirrors curve away from you, and have NEGATIVE R (think of the outside of the ball). There is a point called the FOCAL POINT which is halfway between the mirror and the center. C R R C Concave Mirror R is positive Convex Mirror R is negative

5 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2)

6 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Ray through the center Optical Axis Focal Point

7 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Ray through the center Optical Axis Ray reflects directly back Focal Point

8 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Optical Axis Ray 2 through the focal point Focal Point

9 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Ray 2 reflects parallel to axis Optical Axis Ray 2 through the focal point Focal Point

10 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Focal Point Optical Axis Ray 3 comes in parallel to axis

11 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Here are the rays for a CONCAVE mirror: Ray 3 reflects through focal point Focal Point Optical Axis Ray 3 comes in parallel to axis

12 We will learn 2 techniques for dealing with mirrors (and lenses): Graphical draw the light rays and see where they intersect to find an image. Formula use a couple of formulas to locate and describe an image. First the Graphical Method: For a spherical mirror there are 3 basic rays that you can draw: ) Any ray that goes through the CENTER of the circle reflects directly back toward the light source. 2) Any ray that goes through the FOCAL POINT is reflected back PARALLEL to the optical axis. 3) Any ray that starts parallel to the optical axis is reflected back through the focal point. (opposite of 2) Now here are all 3 rays with an object and its image (at the intersection) Image Optical Axis Object 2 3

13 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it?

14 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? We have a few basic formulas for spherical mirrors. ) The focal length is half the radius. R f = 2 Remember the sign convention if the mirror is concave R is positive. If convex, R is negative.

15 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? We have a few basic formulas for spherical mirrors. ) The focal length is half the radius. R f = 2 2) This formula relates the object (S) and image (S ) positions to the focal length (f) of the mirror. f = S + S' Here S is always positive for mirrors, and S is positive if the image is on the same side as the object (a REAL image). To remember this, just follow the light a real (positive) image will have light rays passing through it.

16 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? We have a few basic formulas for spherical mirrors. ) The focal length is half the radius. R f = 2 2) This formula relates the object (S) and image (S ) positions to the focal length (f) of the mirror. 3) The magnification (m) of the image is related to the relative positions of the object and image. f = S + S' S' m= Don t forget the negative sign in this S formula. The sign of m tells you if the image is upright (+) or inverted (-)

17 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? OK, back to the problem. We have some given information: focal length R=+ 0.5m f =+ 0.25m S=+ 0.2m object distance

18 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? OK, back to the problem. We have some given information: Now we can use formula 2 to locate the image (S ) = + f S S' = S' S' = m R=+ 0.5m f =+ 0.25m S=+ 0.2m object distance focal length

19 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? OK, back to the problem. We have some given information: Now we can use formula 2 to locate the image (S ) = + f S S' = S' S' = m R=+ 0.5m f =+ 0.25m S=+ 0.2m object distance This means the image will be located m BEHIND the mirror. This is a VIRTUAL image. focal length

20 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? OK, back to the problem. We have some given information: Now we can use formula 2 to locate the image (S ) = + f S S' = S' S' = m R=+ 0.5m f =+ 0.25m S=+ 0.2m object distance This means the image will be located m BEHIND the mirror. This is a VIRTUAL image. focal length For the magnification, just use formula 3. S' m m = = = + 5 S 0.2m

21 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? OK, back to the problem. We have some given information: Now we can use formula 2 to locate the image (S ) = + f S S' = S' S' = m R=+ 0.5m f =+ 0.25m S=+ 0.2m object distance This means the image will be located m BEHIND the mirror. This is a VIRTUAL image. focal length For the magnification, just use formula 3. S' m m = = = + 5 S 0.2m So the image is upright (+) and 5 times as large as the object. We could also draw the ray diagram

22 Example using the Formula Method: A concave makeup mirror with radius of curvature 0.5m is held 0.2m from a woman s face. Where is her image and how large is it? Notice the 3 rays in the diagram. They all start at the object and go toward the mirror. Ray through the center is easy to draw. So is ray 2, which starts out flat, then bounces off the mirror and goes through the focal point (f). Ray 3 is the tricky one. Since the object is inside the focal point (closer to the mirror, or S<f) we can t draw the ray through the focal point. Instead we pretend the ray came from the focal point and passed through the object on its way to the mirror, then bounced off flat. The outgoing rays do not intersect! So we have to trace them backwards to find their intersection point behind the mirror. This is what your brain does for you every time you look in a mirror. The virtual image appears at the point where the outgoing light rays seem to be coming from. 3 Object Image f S S 2

23 Convex Mirrors These will work the same way as concave, but R and f are negative. Take a look at where the center of the sphere is it is behind the mirror. There are no light rays there. This is why the radius is negative. Because the light rays do not go there. The 3 typical light rays are shown. Ray points toward the center and bounces straight back. Ray 2 starts flat and bounces off as if it is coming from the focal point. Ray 3 starts toward the focal point and bounces off flat. 3 object R f C Image (this is a virtual image behind the mirror, so S is negative) 2 Convex Mirror R is negative

24 SPHERICAL MIRROR EQUATIONS AND SIGN CONVENTION Light In Side S > 0 Real Object Concave Mirror Illustrated S < 0 Virtual Object C F V Optic Axis Light Out Side S > 0 Real Image C This Side, R > 0 S < 0 Virtual Image C This Side, R < 0 Definitions: C Center of Curvature R Radius of Curvature F Focal Point (Same Side as C) V Vertex Equations: Paraxial Approximation R f = 2 m= y' S' = y S S + S' = f

25 THIN LENS EQUATIONS AND SIGN CONVENTION Surface Surface 2 Light In Side S > 0 Real Object S < 0 Virtual Image C This Side, R < 0 C 2 This Side, R 2 < 0 Light Out Side S < 0 Virtual Object S > 0 Real Image C This Side, R > 0 C 2 This Side, R 2 > 0 n Index of Refraction Definitions: C Center of Curvature, Surface C 2 Center of Curvature, Surface 2 Illustrated Lens is Double Convex Converging With C on the Light Out Side and C 2 on the Light In Side Equations: f = (n ) R R 2 S + S' = f m= y' S' = y S

26 REFRACTION AT SPHERICAL INTERFACE BETWEEN TWO OPTICAL MATERIALS Light In Side S > 0 Real Object S < 0 Virtual Image C This Side, R < 0 n a Index of Refraction Light Out Side S < 0 Virtual Object S > 0 Real Image C This Side, R > 0 n b Index of Refraction Illustrated Interface Has C, Center of Curvature, On The Light Out Side, Thus R > 0 A Flat Interface Has R = n a S nb + S' nb n = R a m= y' nas' = y n S b