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Lecture 14 Images Chp. 35 Opening Demo Topics –Plane mirror, Two parallel mirrors, Two plane mirrors at right angles –Spherical mirror/Plane mirror comparison.

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Presentation on theme: "Lecture 14 Images Chp. 35 Opening Demo Topics –Plane mirror, Two parallel mirrors, Two plane mirrors at right angles –Spherical mirror/Plane mirror comparison."— Presentation transcript:

1 Lecture 14 Images Chp. 35 Opening Demo Topics –Plane mirror, Two parallel mirrors, Two plane mirrors at right angles –Spherical mirror/Plane mirror comparison in forming image –Spherical refracting surfaces –Thin lenses –Optical Instruments Magnifying glass, Microscope, Refracting telescope Warm-up problem

2 Geometrical Optics: Study of reflection and refraction of light from surfaces using the ray approximation. 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. Reflection Refraction: Snells Law n1n2n1n2 Using Fermat’s Principle you can prove the above two laws. 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.

3 Plane mirrors Normal Angle of incidence Angle of reflection i = - p Real sideVirtual side Virtual image

4 Problem: Two plane mirrors make an angle of 90 o. How many images are there for an object placed between them? object eye 1 2 3 mirror

5 Problem: Two plan mirrors make an angle of 60 o. Find all images for a point object on the bisector. object 2 4 5,6 3 1 mirror

6 How tall must be a mirror be for a person to see his entire reflection in it. Let H be the height of a man and let l be the height of the mirror?

7 What happens if we bend the mirror? i = - p magnification = 1 Concave mirror. Image gets magnified. Field of view is diminished Convex mirror. Image is reduced. Field of view increased.

8 Thin Lenses: thickness is small compared to object distance, image distance, and radius of curvature. Converging lens Diverging lens

9 Thin Lens Equation Lensmaker Equation What is the sign convention?

10 Sign Convention p Virtual side - V Real side - R i Light 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 o the V side. r2r2 r1r1

11 Rules for drawing rays to locate images 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.

12 Show Fig 35-14 figure overhead Then go to example

13 24(b). Given a lens with a focal length f = 5 cm and object distance p = +10 cm, find the following: i and m. Is the image real or virtual? Upright or inverted? Draw 3 rays. Image is real, inverted... F1F1 F2F2 p Virtual side Real side

14 24(e). Given a lens with the properties (lengths in cm) r 1 = +30, r 2 = -30, p = +10, and n = 1.5, find the following: f, i and m. Is the image real or virtual? Upright or inverted? Draw 3 rays. Image is virtual, upright. Virtual side Real side r1r1.. F1F1 F2F2 p r2r2

15 27. A converging lens with a focal length of +20 cm is located 10 cm to the left of a diverging lens having a focal length of -15 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. f1f1 f1f1 Lens 1Lens 2 f2f2 f2f2 10 40 +20-15

16 f1f1 f1f1 Lens 1Lens 2 f2f2 f2f2 10 40 +20-15 Ignoring the diverging lens (lens 2), the image formed by the converging lens (lens 1) is located at a distance 40 This image now serves as a virtual object for lens 2, with p 2 = - (40 cm - 10 cm) = - 30 cm. 30 Since m = -i 1 /p 1 = - 40/40= - 1, the image is inverted

17 Thus, the image formed by lens 2 is located 30 cm to the left of lens 2. It is virtual (since i 2 < 0). f1f1 f1f1 Lens 1Lens 2 f2f2 f2f2 10 40 +20-15 40 30 The magnification is m = (-i 1 /p 1 ) x (-i 2 /p 2 ) = (-40/40)x(30/-30) =+1, so the image has the same size orientation as the object.

18 Optical Instruments Magnifying lens Compound microscope Refracting telescope


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