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• textbook sections 28-1 -- 28-3 Physics 1161: Lecture 20 Interference

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Physics 1161: Lecture 20 Interference. textbook sections 28-1 -- 28-3. +1. t. -1. +1. t. -1. +2. t. -2. Superposition. Constructive Interference. +. In Phase. +2. t. -2. Superposition. Destructive Interference. +1. t. -1. +. +1. Out of Phase 180 degrees. t. -1. - PowerPoint PPT Presentation

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Page 1: textbook sections 28-1 --  28-3

• textbook sections 28-1 -- 28-3

Physics 1161: Lecture 20Interference

Page 2: textbook sections 28-1 --  28-3

Superposition

t

+1

-1

t

+1

-1

t

+2

-2

+

Constructive Interference

In Phase

Page 3: textbook sections 28-1 --  28-3

Superposition

t

+1

-1

t

+1

-1

t

+2

-2

+

Destructive Interference

Out of Phase180 degrees

Page 4: textbook sections 28-1 --  28-3

Which type of interference results from the superposition of the two waveforms shown?

1 2 3

0% 0%0%

1. Constructive2. Destructive3. Neither+

Different f

-1.5

-1

-0.5

0

0.5

1

1.5

-1.5

-1

-0.5

0

0.5

1

1.5

Page 5: textbook sections 28-1 --  28-3

Which type of interference results from the superposition of the two waveforms shown?

1 2 3

0% 0%0%

1. Constructive2. Destructive3. Neither+

Different f

-1.5

-1

-0.5

0

0.5

1

1.5

-1.5

-1

-0.5

0

0.5

1

1.5

-2

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

Page 6: textbook sections 28-1 --  28-3

Interference for Light …• Can’t produce coherent light from separate

sources. (f 1014 Hz)

Single source

Two different paths

Interference possible here

• Need two waves from single source taking two different paths– Two slits– Reflection (thin films)– Diffraction*

Page 7: textbook sections 28-1 --  28-3

Coherent & Incoherent Light

Page 8: textbook sections 28-1 --  28-3

Double Slit Interference Applets

• http://www.walter-fendt.de/ph14e/doubleslit.htm

• http://vsg.quasihome.com/interfer.htm

Page 10: textbook sections 28-1 --  28-3

Young’s Double Slit Layout

Page 11: textbook sections 28-1 --  28-3

Interference - Wavelength

Page 12: textbook sections 28-1 --  28-3

Light waves from a single source travel through 2 slits before meeting at the point shown on the screen. The interference will be:

1 2 3

0% 0%0%

1. Constructive2. Destructive3. It depends on L

Screen a distance L from slits

Single source of monochromatic light

d

2 slits-separated by d

L

Page 13: textbook sections 28-1 --  28-3

Light waves from a single source travel through 2 slits before meeting at the point shown on the screen. The interference will be:

1 2 3

0% 0%0%

1. Constructive2. Destructive3. It depends on L

Screen a distance L from slits

Single source of monochromatic light

d

2 slits-separated by d

L

The rays start in phase, and travel the same distance, so they will arrive in phase.

Page 14: textbook sections 28-1 --  28-3

Young’s Double SlitCheckpoint

Screen a distance L from slits

Single source of monochromatic light

d

2 slits-separated by d

1) The pattern of maxima and minima is the same for original and modified experiments.

2) Maxima and minima for the unmodified experiment now become minima and maxima for the modified experiment.

L

½ shift

The experiment is modified so that one of the waves has its phase shifted by ½ . Now, the interference will be:

Page 15: textbook sections 28-1 --  28-3

Young’s Double SlitCheckpoint

Screen a distance L from slits

Single source of monochromatic light

d

2 slits-separated by d

1) The pattern of maxima and minima is the same for original and modified experiments.

2) Maxima and minima for the unmodified experiment now become minima and maxima for the modified experiment.

L

½ shift

The experiment is modified so that one of the waves has its phase shifted by ½ . Now, the interference will be:

For example at the point shown, he rays start out of phase and travel the same distance, so they will arrive out of phase.

Page 16: textbook sections 28-1 --  28-3

Young’s Double Slit Concept

Screen a distance L from slits

Single source of monochromatic light

d

2 slits-separated by d

L

At points where the difference in path length is 0, ,2, …, the screen is bright. (constructive)

At points where the difference in path

length is

the screen is dark. (destructive)

2

5 ,2

3 ,2

Page 17: textbook sections 28-1 --  28-3

Young’s Double Slit Key IdeaL

Two rays travel almost exactly the same distance. (screen must be very far away: L >> d)

Bottom ray travels a little further.

Key for interference is this small extra distance.

Page 18: textbook sections 28-1 --  28-3

d

Path length difference =

d

Young’s Double Slit Quantitative

Destructive interference dsin (m

12)

Constructive interference dsin m

where m = 0, or 1, or 2, ...

d sin

Need < d

Page 19: textbook sections 28-1 --  28-3

d

Destructive interference dsin (m

12)

Constructive interference dsin m

where m = 0, or 1, or 2, ...

Young’s Double Slit Quantitative

y

sin() tan() = y/L

dLmy

d

Lmy

21

L

A little geometry…

Page 20: textbook sections 28-1 --  28-3

Young’s Double Slit Under WaterCheckpoint

d

L

y

When this Young’s double slit experiment is placed under water, how does the pattern of minima and maxima change?

1) the pattern stays the same

2) the maxima and minima occur at smaller angles

3) the maxima and minima occur at larger angles

Page 21: textbook sections 28-1 --  28-3

Young’s Double Slit Under WaterCheckpoint

d

L

y

When this Young’s double slit experiment is placed under water, how does the pattern of minima and maxima change?

1) the pattern stays the same

2) the maxima and minima occur at smaller angles

3) the maxima and minima occur at larger angles…wavelength is shorter under water.

Page 22: textbook sections 28-1 --  28-3

Young’s Double SlitCheckpoint

In Young’s double slit experiment, is it possible to see interference maxima when the distance between slits is smaller than the wavelength of light?

1) Yes 2) No

Page 23: textbook sections 28-1 --  28-3

Young’s Double Slit CheckpointIn Young’s double slit experiment, is it possible to see interference maxima when the distance between slits is smaller than the wavelength of light?

1) Yes 2) No

Need: d sin = m => sin = m / d

If > d then / d > 1

so sin > 1

Not possible!

Page 24: textbook sections 28-1 --  28-3

Reflections at Boundaries

Free End ReflectionNo phase change

Slow Mediumto

Fast Medium

Fast Mediumto

Slow Medium

Fixed End Reflection180o phase change

Page 25: textbook sections 28-1 --  28-3

Newton’s Rings

Page 26: textbook sections 28-1 --  28-3

Iridescence

Page 27: textbook sections 28-1 --  28-3

Iridescence

Page 28: textbook sections 28-1 --  28-3

Soap Film Interference• This soap film varies in

thickness and produces a rainbow of colors.

• The top part is so thin it looks black.

• All colors destructively interfere there.

Page 29: textbook sections 28-1 --  28-3

Thin Film Interference

n1 (thin film)

n2

n0=1.0 (air)

t

1 2

Get two waves by reflection from the two different interfaces.

Ray 2 travels approximately 2t further than ray 1.

Page 30: textbook sections 28-1 --  28-3

Reflection + Phase Shifts

n1

n2

Upon reflection from a boundary between two transparent materials, the phase of the reflected light may change.

• If n1 > n2 - no phase change upon reflection.

• If n1 < n2 - phase change of 180º upon reflection. (equivalent to the wave shifting by /2.)

Incident wave Reflected wave

Page 31: textbook sections 28-1 --  28-3

Thin Film Summary

n1 (thin film)

n2

n = 1.0 (air)

t

1 2

Ray 1: d1 = 0 or ½

Determine d, number of extra wavelengths for each ray.

If |(d2 – d1)| = ½ , 1 ½, 2 ½ …. (m + ½) destructiveIf |(d2 – d1)| = 0, 1, 2, 3 …. (m) constructive

Note: this is wavelength in film!

(film= o/n1)+ 2 t/ film

Reflection Distance

Ray 2: d2 = 0 or ½

This is important!

Page 32: textbook sections 28-1 --  28-3

Thin Film Practice

nglass = 1.5

nwater= 1.3

n = 1.0 (air)

t

1 2

d1 =

d2 =

Blue light (o = 500 nm) incident on a glass (nglass = 1.5) cover slip (t = 167 nm) floating on top of water (nwater = 1.3).

Is the interference constructive or destructive or neither?

Phase shift = d2 – d1 =

Page 33: textbook sections 28-1 --  28-3

Thin Film Practice

nglass = 1.5

nwater= 1.3

n = 1.0 (air)

t

1 2

d1 = ½

d2 = 0 + 2t / glass = 2t nglass/ 0= 1

Blue light (o = 500 nm) incident on a glass (nglass = 1.5) cover slip (t = 167 nm) floating on top of water (nwater = 1.3).

Is the interference constructive or destructive or neither?

Phase shift = d2 – d1 = ½ wavelength

Reflection at air-film interface only

Page 34: textbook sections 28-1 --  28-3

Blue light = 500 nm incident on a thin film (t = 167 nm) of glass on top of plastic. The interference is:

1 2 3

0% 0%0%

nglass =1.5

nplastic=1.8

n=1 (air)

t

21

1. Constructive2. Destructive3. Neither

Page 35: textbook sections 28-1 --  28-3

Blue light = 500 nm incident on a thin film (t = 167 nm) of glass on top of plastic. The interference is:

1 2 3

0% 0%0%

nglass =1.5

nplastic=1.8

n=1 (air)

t

21

1. Constructive2. Destructive3. Neither

d1 = ½ d2 = ½ + 2t / glass = ½ + 2t nglass/ 0= ½ + 1

Phase shift = d2 – d1 = 1 wavelength

Page 36: textbook sections 28-1 --  28-3

Thin FilmsCheckpoint

The gas looks: • bright • dark

A thin film of gasoline (ngas=1.20) and a thin film of oil (noil=1.45) are floating on water (nwater=1.33). When the thickness of the two films is exactly one wavelength…

t =

nwater=1.3

ngas=1.20

nair=1.0

noil=1.45

The oil looks: • bright • dark

Page 37: textbook sections 28-1 --  28-3

Thin FilmsCheckpoint

The gas looks: • bright• dark

A thin film of gasoline (ngas=1.20) and a thin film of oil (noil=1.45) are floating on water (nwater=1.33). When the thickness of the two films is exactly one wavelength…

t =

nwater=1.3

ngas=1.20

nair=1.0

noil=1.45

d1,gas = ½

The oil looks: • bright• dark

d2,gas = ½ + 2 d1,oil = ½ d2,oil = 2| d2,gas – d1,gas | = 2 | d2,oil – d1,oil | = 3/2

constructive destructive