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Physics 7E Prof. D. Casper
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Admin Chapter 34 HW is due a week from today (Monday, 7 am) Reading
Due to my mistake, it has only been available since 7am today – sorry! Reading Wednesday: Chapter 35.1 – 35.3 Next Monday: Chapter 35.4 – 35.5 Week 9 10 Finals Monday Tuesday Wednesday Thursday Friday 34.5 – 34. 8 35.1 – 35.3 Thanksgiving 35.4 – 35.5 Ch. 34 HW Due Ch. 36 Lecture Ch. 35 HW Due Ch. 36 HW Due Final (8am)
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Concave Mirror: Ray Tracing
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Convex Mirror: Ray Tracing
1 𝑠 + 1 𝑠 ′ = 1 𝑓 → 1 𝑠 ′ = 1 𝑓 − 1 𝑠 if 𝑓<0 and 𝑠>0, then 𝑠 ′ <0 Real object always forms virtual image in convex mirror
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Concave Mirror: Real and Virtual Images
In these examples: 𝑅=20 cm, 𝑓=10 cm 𝑠=30 cm: 𝑠 ′ = 1 10 → 𝑠 ′ =15 cm 𝑚=− 𝑠 ′ 𝑠 =− 1 2 (real, inverted image) 𝑠=20 cm: 𝑠 ′ = 1 10 → 𝑠 ′ =20 cm 𝑚=− 𝑠 ′ 𝑠 =−1 (real, inverted image) 𝑠=10 cm: 𝑠 ′ = 1 10 → 𝑠 ′ →∞ (no image) 𝑠=5 cm: 𝑠 ′ = 1 10 → 𝑠 ′ =−10 cm 𝑚=− 𝑠 ′ 𝑠 =+2 (virtual, upright image)
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A. real and larger than the object.
Q34.3 An object is placed 4.0 m away from a concave mirror of focal length +1.0 m. The image formed by the mirror is A. real and larger than the object. B. real and smaller than the object. C. real and the same size as the object. D. virtual and larger than the object. E. virtual and smaller than the object. Answer: B
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A. real and larger than the object.
An object is placed 4.0 m away from a concave mirror of focal length +1.0 m. The image formed by the mirror is A. real and larger than the object. B. real and smaller than the object. C. real and the same size as the object. D. virtual and larger than the object. E. virtual and smaller than the object.
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A. real and larger than the object.
Q34.7 An object is placed 2.0 m away from a convex mirror of focal length –1.0 m. The image formed by the mirror is A. real and larger than the object. B. real and smaller than the object. C. real and the same size as the object. D. virtual and larger than the object. E. virtual and smaller than the object. Answer: E
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A. real and larger than the object.
An object is placed 2.0 m away from a convex mirror of focal length –1.0 m. The image formed by the mirror is A. real and larger than the object. B. real and smaller than the object. C. real and the same size as the object. D. virtual and larger than the object. E. virtual and smaller than the object.
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Summary of Mirror Images
For a REAL object: Plane Mirror Image always virtual and upright (| 𝑠 ′ |=𝑠,𝑚=1) Convex Mirror Image always virtual and upright (| 𝑠 ′ |<𝑠, 0<𝑚<1) Concave Mirror If 𝑠<𝑓: Image virtual and upright (𝑚>1) If 𝑠>𝑓: Image real and inverted (𝑚<0) If 𝑠=𝑓, no image
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Spherical Refracting Surface: Paraxial Approximation
𝑛 𝑎 𝑠 + 𝑛 𝑏 𝑠 ′ = 𝑛 𝑏 − 𝑛 𝑎 𝑅 𝑚= 𝑦 ′ 𝑦 =− 𝑛 𝑎 𝑠 ′ 𝑛 𝑏 𝑠 Center on side with outgoing light: 𝑅>0 Center not on side with outgoing light: 𝑅<0
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Lens Properties Thicker in middle focal length 𝑓>0
Thinner in middle focal length 𝑓<0
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Thin Lens Equation 1 𝑠 + 1 𝑠 ′ = 1 𝑓
1 𝑠 + 1 𝑠 ′ = 1 𝑓 Sign conventions are all-important! s > 0: Object on side with incoming light s’ > 0: Image on side with outgoing light f > 0: Converging lens Lateral magnification: 𝑚= 𝑦 ′ 𝑦 =− 𝑠 ′ 𝑠
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Ray-tracing: Converging Lens
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Ray tracing: Diverging Lens
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Multiple Lens Systems For multiple lenses and/or mirrors, you take
one element at a time. The image of one element is the object of the next In the diagram, we have two converging lenses with 𝑓 1 =8.0 cm and 𝑓 2 =6.0 cm a distance 36.0 cm apart Find the image of O in Lens A (ignoring Lens B for now): 𝑠 1 ′ = 1 8 → 𝑠 1 ′ =24 cm What is the object distance for Lens B? 𝑠 2 =36 cm−24 cm=12 cm 𝑠 2 ′ = 1 6 → 𝑠 2 ′ =12 cm 𝑚= 𝑚 1 × 𝑚 2 =(−2)×(−1)=+2
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“Virtual” Objects In the previous example, the image of Lens A was “in front” of Lens B (on the side the light entered Lens B) It is possible to have the opposite situation Suppose both lenses have f = 10 cm, they are 10 cm apart, and the object is 20 cm from Lens A ( 𝑠 1 =20) The image in Lens A will then be 20 cm to the right of Lens A (and 10 cm to the right of B) Since it is not on the side the light enters B, the object distance for Lens B is -10 cm 1 − 𝑠 2 ′ = 1 10 → 𝑠 2 ′ =+20 cm Image of Object In Lens A Image of Object In Lens B Object Virtual Object For Lens B Lens A Lens B
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Lens-maker’s Equation
The focal length of a lens can be worked out by treating the image of its front face as the object for its back face See the book for a full derivation The focal length depends on the curvature of the two surfaces, and the index for refraction of the material For a thin lens, the result is: 1 𝑓 = 𝑛− 𝑅 1 − 1 𝑅 2
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