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Interference: Phase Differences and Coherence in Wave Systems, Slides of Electrical Engineering

The concept of interference in wave systems, focusing on phase differences and coherence length. It covers constructive and destructive interference, the intensity of two interfering waves, and the ways in which the phase difference between two waves can change, including through different indexes of refraction, path lengths, and reflection from a boundary. The document also includes a demo using a soap bubble and a question about reflection phase shifts.

Typology: Slides

2012/2013

Uploaded on 08/20/2013

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LECTURE 26: Interference
http://content.answers.com/main/content/img/CDE/_CDVSDVD.GIF
http://www.sonic.net/~ideas/graphics/mma_cd.gif6
4/18/12 2
Interference
When two waves with the same frequency f and
wavelength combine, the resultant is a wave whose
amplitude depends on the phase different, .
4/18/12 3
Interference: Phase Differences
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0 20 40 60 80 100
Amplitude (arbitrary units)
Position (arbitrary units)
-4
-3
-2
-1
0
1
2
3
4
0 20 40 60 80 100
Amplitude (arbitrary units)
Position (arbitrary units)
-3
-2
-1
0
1
2
3
0 20 40 60 80 100
Amplitude (arbitrary units)
Position (arbitrary units)
= 0 or 1#
= 0.5 #
= 0.3 #
Constructive
Interference
Destructive
Interference
4/18/12 4
Coherence
Infinite coherence length
Finite coherence
length
Single Photon
pf3
pf4
pf5

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LECTURE 26: Interference

http://content.answers.com/main/content/img/CDE/_CDVSDVD.GIF http://www.sonic.net/~ideas/graphics/mma_cd.gif 4/18/12 2

Interference

When two waves with the same frequency f and wavelength  combine, the resultant is a wave whose amplitude depends on the phase different, . 4/18/12 3

Interference: Phase Differences

-1.

-0. 0

1

2 0 20 40 60 80 100 Amplitude (arbitrary units) Position (arbitrary units)

0 1 2 3 4 0 20 40 60 80 100 Amplitude (arbitrary units) Position (arbitrary units)

0 1 2 3 0 20 40 60 80 100 Amplitude (arbitrary units) Position (arbitrary units)  = 0 or 1 #  = 0.5 #  = 0.3 # Constructive Interference Destructive Interference 4/18/12 4

Coherence

Infinite coherence length Finite coherence length

Single Photon

4/18/12 5

Intensity of Two Interfering Waves

*Two light waves not in phase:

E 1 = Eo sin ω t

E 2 = Eo sin( ω t + δ )

4/18/12 6

Intensity of Two Interfering Waves

*Maxima occur for: δ = 2 m π

*Minima occur for: δ = ( 2 m + 1 ) π

for m = 0, 1, 2, 3…. 4/18/12 7

Interference

*Three ways in which the phase difference between two waves can change:

  1. By traveling though media of different indexes of refraction
  2. By traveling along paths of different lengths
  3. By reflection from a boundary 4/18/12 8

Interference: Different Indexes of Refraction

*The phase difference between two waves can change if the waves travel through different material having different indexes of refraction. n 1 n 2

N 2 − N 1 =

L

( n 2 − n 1 ) L

4/18/12 13

Interference: Reflection from a Boundary

*The phase difference between two waves can change if one or both are reflected. Reflection Reflection Phase Shift Off lower index zero Off higher index 0.5# 4/18/12 14

Interference: Reflection from a Boundary

*The phase difference between two waves can change if one or both are reflected. DEMO: Soap Bubble Colored interference fringes will be seen on the screen. light beam projector mirror screen soap film 4/18/12 15 QUESTION: Which ray experiences a shift due to reflection? a) Ray 1 b) Ray 2 c) none d) both

Interference: Reflection from a Boundary

*The phase difference between two waves can change if one or both are reflected. Reflection Reflection Phase Shift Off lower index zero Off higher index 0.5# 4/18/12 16

Interference: Soap Bubble

The phase difference between the two waves is caused by:

  1. Phase shift on reflection for for ray 1 of 0.5 . Ray 2 does not phase shift on reflection.
  2. Path length difference between ray 1 & ray 2 is 2t. Ray 2 crosses the film twice. For in-phase waves (maxima - bright fringes): For out of-phase waves (minima - dark fringes): Valid for n 2 > n 1 and n 2 > n 3

2 t = ( m +

n 2

2 t = m

λ

n 2

The total difference between ray 1 and ray 2 is the extra difference traveled plus the shift due to reflection.

4/18/12 17

Interference of Reflections from a film of water

4/18/12 18

Interference of Reflections from a film of water

δ from path length difference =

2 t

⎝⎜^

⎠⎟^

2 π, where λ ' =

n

Ray 1: 1800 phase shift from reflection off water surface Ray 2: no phase change going into the water, 180^0 phase change upon reflection from glass. Since both rays are shifted upon reflection the overall difference between the two rays is just the extra path traveled:

∴ constructive interference for 2 t = m λ ', m = 0 , 1 , 2 , 3 ,...

destructive interference for 2 t = m +

⎝⎜^

λ ', m = 0 , 1 , 2 , 3...

4/18/12 19

Newton’s Rings

no phase change 1800 phase ~ zero path change optical flat length difference 4/18/12 20

Newton’s Rings:

Poor quality Excellent quality

Fringes from a wedge-shape film of air indicating how optically flat are the glass plates.