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**Announcements Homework for tomorrow… (Ch. 23, CQ7, Probs. 32 & 33)**

FINAL EXAM: PHYS (10 am class): Monday, May 10-11:50 am PHYS (11 am class): Wednesday, May 10-11:50 am Homework for tomorrow… (Ch. 23, CQ7, Probs. 32 & 33) CQ6: red, black 23.16: 23 cm 23.18: 113 cm 23.53: 1.1° Office hours… MW 12:30-1:30 pm TR am F am Tutorial Learning Center (TLC) hours: M 8-1 pm, 3-6 pm, W 8-1 pm, 2-6 pm TR 8-6 pm, F 8-2 pm

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**Ray Optics (Thin Lenses: Ray Tracing & Refraction Theory)**

Chapter 23 Ray Optics (Thin Lenses: Ray Tracing & Refraction Theory)

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**Last time… Rayleigh Scattering…**

Ray Tracing through a thin converging lens… A parallel ray will go through the far focal point after passing through the lens. A ray through the near focal point of a thin lens becomes parallel after passing through the lens. A ray through the center of a thin lens travels in a straight line.

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**Lateral Magnification…**

The image can be either larger or smaller than the object, depending on the location and focal length of the lens. The lateral magnification, m, is defined as: Notice: Positive m = upright image. Negative m = inverted image. The absolute value of m gives the size ratio of the image and object: h/h |m|.

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Virtual Images… Consider a converging lens for which the object is inside the focal point, at distance s < f. All 3 rays appear to diverge from point P. Point P is an upright, virtual image of the object point P. Notice: Image distance s’ for a virtual image is negative.

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**i.e. 23.9: Magnifying a flower**

To see a flower better, a naturalist holds a 6.0 cm focal length magnifying glass 4.0 cm from the flower. What is the magnification?

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**23.6 Thin Lenses: Ray Tracing**

3 situations form the basis for ray tracing through a thin diverging lens. A ray initially parallel to the optical axis will appear to diverge from the near focal point after passing through the lens. A ray directed along a line toward the far focal point becomes parallel to the optical axis after passing through the lens. A ray through the center of a thin lens is neither bent nor displaced but travels in a straight line.

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**i.e. 23.10 De-magnifying a flower**

A diverging lens with a focal length of 50 cm is placed 100 cm from a flower. Where is the image? What is its magnification?

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**23.7: Thin Lenses: Refraction Theory**

Consider a spherical boundary between two transparent media with indices of refraction n1 and n2. The sphere has radius of curvature R and is centered at pt C. If an object is located at distance s from a spherical refracting surface, an image will be formed at distance s given by:

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**23.7: Thin Lenses: Refraction Theory**

Consider a spherical boundary between two transparent media with indices of refraction n1 and n2. The sphere has radius of curvature R and is centered at pt C. If an object is located at distance s from a spherical refracting surface, an image will be formed at distance s given by:

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**23.7: Thin Lenses: Refraction Theory**

If an object is located at distance s from a spherical refracting surface, an image will be formed at distance s given by:

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**i.e. 23.11: Image formation inside a glass rod**

One end of a 4.0 cm diameter glass rod is shaped like a hemisphere. A small light bulb is 6.0 cm from the end of the rod. Where is the bulb’s image located?

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i.e : A goldfish in a bowl A goldfish lives in a spherical fish bowl 50 cm in diameter. If the fish is 10 cm from the near edge of the bowl, where does the fish appear when viewed from the outside?

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i.e : A goldfish in a bowl A goldfish lives in a spherical fish bowl 50 cm in diameter. If the fish is 10 cm from the near edge of the bowl, where does the fish appear when viewed from the outside?

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Chapter 34 Lecture Eight: Images: II. Image Formed by a Thin Lens A thin lens is one whose thickness is small compared to the radii of curvature For a.

Chapter 34 Lecture Eight: Images: II. Image Formed by a Thin Lens A thin lens is one whose thickness is small compared to the radii of curvature For a.

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