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Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab [email protected] Geometrical Optics: Image Formation

Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab [email protected] Geometrical Optics: Image Formation

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Page 1: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Physics 106 Lesson #25

Dr. Andrew Tomasch

2405 Randall Lab

[email protected]

Geometrical Optics:Image Formation

Page 2: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Review: Simple Harmonic Motion (SHM) • For a mass-and-spring

oscillator, the oscillation frequency f is governed by inertia (mass) and the restoring force (spring constant)– A bigger mass produces a

smaller f (slower oscillation → longer period)

– A bigger restoring force (bigger spring constant) produces a bigger f (faster oscillation→shorter period)

1

2

kf

m

k

m

fT 2

1

f is the natural frequency of a mass-and-spring oscillator.

Hooke’s Law: Fspring= -kx

Page 3: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

•The frequency and period are independent of the mass of the pendulum bob• Assuming g is fixed, the only way to change the period is to change the length of the pendulum•A pendulum with a fixed length can be used to measure g → different f, T on a planet with a different g or at different places on Earth

Review: The Simple Pendulum

1 1 2

2

g Lf T

L f g

f is the natural frequency of a simple pendulum.

Page 4: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

• Damping forces are often put into a system deliberately to prevent it from oscillating indefinitely

• Example: the shock absorbers in your car– Too little damping too “bouncy” a ride– Too much damping too “stiff” a ride

• Q: How can you tell if a system is underdamped or overdamped?

A: Disturb it. If it oscillates for a while it’s underdamped. If it returns to the equilibrium position without oscillating it’s overdamped .

Review: Damping

Page 5: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

driving naturalf f

• Natural Frequency: a frequency determined by the physical properties of a vibrating object

• Driving an object at its resonant frequency (≡natural frequency) produces high-amplitude oscillations

• Objects driven at their natural frequency can be damaged or destroyed

Review: Resonance

driving naturalf f

Demo: Mass and Spring on Finger

Page 6: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Propagation of Light Waves

• Light waves arrive at objects and interact with them in three basic ways. They can:

1. Reflect (bounce off)

2. Refract (go through)

3. Be absorbed (stop)

• Not exclusive, all three may occur

Demonstration

Page 7: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

• Diffuse Reflection

Rough surface →

rays reflected in various directions

• Specular Reflection

Smooth mirror-like surface → rays reflected parallel

Reflection

Page 8: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Law of Reflection• The incident ray,

reflected ray and the normal to the surface are all in the same plane.

• The angle of incidence equals the angle of reflection.

i r

Page 9: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

• Light comes in straight lines from the object to you

• Light from different points on the object strikes your retina in different places

• An image is a location at which there is a one-to-one correspondence between points on the object and points on the image.

How Do We See Objects?

Page 10: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Why do you see images only in mirrors, and not, for example, in the wall?

A. Light is not reflected from the wall

B. The law of reflection does not apply to the wall

C. Light does not pass through the wall

D. The wall isn’t flat enough

Concept Test #1

Page 11: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Plane Mirrors• A ray of light from the top of the chess piece reflects

from the mirror • To the eye, the ray seems to come from behind the

mirror• Because none of the rays actually emanate from the

image, it is called a virtual image

Page 12: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Real Images From a Pinhole•The oldest known camera•Used by renaissance artists for one-point perspective drawings•Called the Camera Obscura in classical times

Page 13: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Refraction

• As light passes from one medium to another it changes direction at the interface between the two media

• This change of direction is known as refraction

Page 14: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Index of Refraction

• Light travels through materials at a speed less than its speed in a vacuum

Indices of Refraction

Vacuum 1 (exactly)

Air 1.0003

Water 1.333

Ice 1.309

Glass 1.523

Diamond 2.419

c cn v

v n

INDEX OF REFRACTION

Page 15: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Refraction at Surface of Water

http://www.opticalres.com/gentsupp_f.html

Page 16: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

While boating on the Amazon, you decide to go spear fishing. You look into the water and see where a fish appears to be. Where should you aim your spear?

1) Beyond where the fish appears

2) In front of where the fish appears

3) Directly where the fish appears

Concept Test #2

Where the fish really is

Where the fish really is

What you see

Page 17: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Secret of the Archer Fish

• Shot with a powerful jet of water, the prey falls into the water and the Archer Fish swims to the surface to retrieve its meal.

• The secret to the Archer Fish's success is that it lines up its aim from a position directly underneath the prey.

Page 18: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Thin Lenses• Lenses refract light in such a way that

an image of the light source is formed

• Two types of lenses: converging (convex) and diverging (concave)

Converging Lens Diverging Lens

Page 19: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

A Thin Converging Lens Produces a Real, Inverted Image for Objects Outside the Focal Length

A Thin Converging Lens Has a Positive Focal Length-a Real Image can be Produced on the Side Opposite the Object.

Page 20: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

A Thin Converging Lens Produces a Virtual, Upright Image for Objects Inside the Focal Length

Page 21: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

A Thin Diverging Lens Produces a Virtual, Upright Image for Objects Outside the Focal Length

A Thin Diverging Lens Has a Negative Focal Length—the Image Appears on the Same Side as the Object. A Diverging Lens Cannot Form a Real Image

Page 22: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Thin Lens Equation

•Relates the Image Distance (i), the Object Distance (o) and the Focal Length (f)•Works for both Converging and Diverging lenses provided the focal length for a Diverging lens is defined to be negative.

1 1 1

i o f

Page 23: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

f f

f/22 Lensf/3 Lens

Object Object

FilmFilm

Lens

A Typical Camera

Two Cameras With Different f/numbers

Page 24: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Dispersion• The index of refraction for a given material will vary

with the wavelength of the light passing through it• This means that different colors of light will be

refracted through different angles when passing through the same medium.

• This is called dispersion and can be demonstrated with a prism or by observing a rainbow

Page 25: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Spectrum of a Prism

White light is a combination of all the visible colors

nr< no < ny < ng < nb < ni <nv

Page 26: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

Rainbows• Rainbows are a spectacular example of

dispersion by droplets of water in the air when the the sun is at your back

• Rainbows can be observed when sunlight is refracted and then reflected off the back surface of water droplets

Page 27: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

The Secondary Rainbow

• A secondary rainbow is caused by light which reflects twice inside the drop

• The colors in the secondary rainbow are reversed!

Primary RainbowSecondary Rainbow

Page 28: Physics 106 Lesson #25 Dr. Andrew Tomasch 2405 Randall Lab atomasch@umich.edu Geometrical Optics: Image Formation

A Double Rainbow…