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Physics 1B03summer-Le cture 10 Interference of Waves Beats Double Slit

Interference of Waves Beats Double Slit

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Interference of Waves Beats Double Slit. Beats. Two waves of different frequencies arriving together produce a fluctuation in power or amplitude. Since the frequencies are different, the two vibrations drift in and out of phase with each other, causing the total amplitude to vary with time. - PowerPoint PPT Presentation

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Page 1: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Interference of Waves

BeatsDouble Slit

Page 2: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

BeatsBeats

Two waves of different frequencies arriving together produce a fluctuation in power or amplitude.

Since the frequencies are different, the two vibrations drift in and out of phase with each other, causing the total amplitude to vary with time.

y

time

1 beat

Page 3: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

time

t

in phase 180o out of phase in phase

Page 4: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Same amplitudes, different frequencies:

)cos( 11 tAy )cos( 22 tAy

Trigonometry: cos a + cos b = 2 cos [(a-b)/2] cos [(a+b)/2]

Result:

ttA

yyy

2cos

2cos2 2121

21

slowly-varyingamplitude

SHM at averagefrequency

The math:

Page 5: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Note:

2 beats per cycle of

t2

cos 21

# beats/second =

22 21 ff

The beat frequency (number of beats per second) is equal to the difference between the frequencies:

21 fffb

Page 6: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Quiz

Two guitar strings originally vibrate at the same 400-Hz frequency. If you hear a beat of 5Hz, what is/are the other possible frequencie(s) ?

a) 10 Hzb) 395 Hzc) 405 Hzd) 395 Hz and 405 Hz

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Physics 1B03summer-Lecture 10

InterferenceInterference

2 waves, of the same frequency; arrive out of phase.

Eg: y1=Asin t y2=Asin (t+)

Then yR= y1 + y2 = AR sin(t+R),

and the resultant amplitude is AR=2Acos(½.

Identical waves which travel different distances will arrive out of phase and will interfere, so that the resultant amplitude varies with location.

Page 8: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Phase difference :

Define

Then, at detector:

rkrrktkrtkr )()()( 2121

(pick starting timeso initial phase is zero here)

cycles) (or

radians2

r

rrk

)2

sin()2

cos2(

)sin(

)sin(

2

1

tAy

tAy

tAy

R

Page 9: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Example:

Two sources, in phase; waves arrive by different paths:

At detector P:

)sin(

)sin(

22

11

tkrAy

tkrAy

detectorS1

S2

Pr1

r2

Page 10: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

8 m

x

2 speakers, in phase; f = 170 Hz (so = 2.0 m; the speed of sound is about 340 m/s)

As you move along the x axis, where is the sound:

a) a minimum (compared to nearby points)?b) a maximum (compared to nearby points)?

detector

Page 11: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Solution:

Page 12: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

10 min rest

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Physics 1B03summer-Lecture 10

Interference of LightInterference of Light

Light is an electromagnetic (EM) wave.

Wave properties:

Diffraction – bends around corners, spreads out from narrow slits

Interference – waves from two or more coherent sources

interfere

Page 14: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Electromagnetic WavesElectromagnetic Waves

Usually we keep track of the electric field E :

Electric field amplitude

all vBE

,,

E B (magnetic field)Eo

)sin(),( tkxtx AE

v

Electromagnetic waves are transverse waves

Page 15: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Infrared

Red 780 nm

Yellow 600 nm

Green 550 nm

Blue 450 nm

Violet 380 nm

Ultraviolet

Visible-LightVisible-Light SpectrumSpectrum

Page 16: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

The Electromagnetic SpectrumThe Electromagnetic Spectrum

(m) f (Hz) 300 106

3 108

3 x 10-3 1011

3 x 10-6 1014

7 x 10-7 5x1014

4 x 10-7

3 x 10-9 1017

3 x 10-12 1020

RadioTV

Microwave

Infrared

Visible

UltravioletX rays rays

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Physics 1B03summer-Lecture 10

Our galaxy (Milky Way) at viewed at different wavelengths

Page 18: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Radio lobes (jets) from a supermassive black hole at the center of the galaxy NGC 4261

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Physics 1B03summer-Lecture 10

Double SlitDouble Slit(Thomas Young, 1801)

Result: Many bright “fringes” on screen, with dark lines in between.

screen

double slit

separation d

θ

m=2m=1

m=0 (center) m=-1 m=-2

incident light

Page 20: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

The slits act as two sources in phase. Due to diffraction, the light spreads out after it passes through each slit. When the two waves arrive at some point P on the screen, they can be in or out of phase, depending on the difference in the length of the paths.

The path difference varies from place to place on the screen. Pr1

r2

Δr = r

1-r2

d

To determine the locations of the bright fringes (interference maxima), we need to find the points for which the path difference r is equal to an integer number of wavelengths.

For dark fringes (minima), the path difference is integer multiples of half of a wavelength.

Page 21: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

For light, the slits will usually be very close together compared to the distance to the screen. So we will place the screen “at infinity” to simplify the calculation.

Pr1

r2

Δr = r

1-r2

d

r >> d, r1 & r2 nearly parallel

d

Δr

θ

θ

Δr = d sin θ

move P to infinity

Page 22: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Interference:Interference: 2 coherent waves, out of phase 2 coherent waves, out of phase due to a path difference due to a path difference r:r:

Constructive Interference (maximum intensity)

for = 0, ±2π, ±4π, ±6π, ……… -> Δr =0, ±, ±2 , ±3 , ………

cycles

radians 2difference phase

r

r

Destructive Interference (minimum intensity)

for = ±π, ±3π, ±5π, ……… -> Δr =±λ/2, ±3λ/2, ±5λ/2, ………

Page 23: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Constructive Interference: (bright)

Δr = mλ ord sin θ = mλ, m = 0, ±1, ±2, …

But, if the slit-screen distance (L) is large, then sinθ~θand so sinθ=θ=y/L (in radians):

L

So we have: mL

dy

d

Page 24: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Destructive Interference: (no light)

Δr = (m + ½)λ ord sin θ = (m + ½) λ, m = 0, ±1, ±2, …

So, we have: )2

1( m

L

dy

Page 25: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Two slits are illuminated with red light to produce an interference patter on a distant screen. If the red light is replaces with blue light, how does the pattern change?

A) The bright spots move closer togetherB) The bright spots move farther apartC) The pattern does not changeD) The patter doesn’t chance, but the width of the

spots changes

Quiz

Page 26: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

ExamplExamplee

Where are a) the bright fringes?b) the dark lines?

(give values of y)

3 m

y

0

2 slits, 0.20 mm apart; red light ( = 667 nm)

screen

Page 27: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Solution:

Page 28: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Example

A double slit interference patter is observed on a screen 1.0m behind two slits spaced 0.3mm apart. Ten bright fringes span a distance of 1.65 cm.

What is the wavelength of light used ?

Page 29: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Which of the following would cause the separation between the fringes to decrease?

A) Increasing the wavelength B) Decreasing the wavelength C) Moving the slits closer together D) Moving the slits farther apart E) None of the above

Quiz

Page 30: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

10 min rest

Page 31: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Refractive IndexRefractive Index

material refractive index speed of light

vacuum 1 c 300,000 km/sair 1.0003glass about 1.5 200,000 km/swater 1.333 225,000 km/sdiamond 2.4 125,000 km/s

The speed of light depends on the material. We define the refractive index “n” as

n = (speed of light in vacuum)/(speed of light in a material)

Page 32: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Question:

A beam of yellow light (wavelength 600 nm), travelling in air, passes into a pool of water. By what factor do the following quantities change as the beam goes from air into water?

A) speed B) frequency C) wavelength

Page 33: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Reflection and Phase Reflection and Phase ChangeChange

Light waves may have a 180° phase change when they reflect from a boundary:

“optically dense” medium (larger refractive index)

no phase change at this reflection180° phase change

when reflecting from a denser medium

Just remember this : low to high, phase shift of pi !

Page 34: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Example: Thin filmExample: Thin film

What is the minimum thickness of a soap film (n 1.33) needed to produce constructive interference for light with a 500nm wavelength ? (air : n 1.00).

What about destructive interference ?

Page 35: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

Example: Antireflection Example: Antireflection coatingscoatings

To reduce reflections from glass lenses (n 1.5), the glass surfaces are coated with a thin layer of magnesium fluoride (n 1.38). What is the correct thickness of the coating for green light (550 nm vacuum wavelength)?

MgF2air glass

Page 36: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

ExampleExample

A beam of 580 nm light passes through two closely spaced glass plates (nglass=1.6), as shown in the figure below. For what minimum nonzero value of the plate separation d is the transmitted light dark?

Page 37: Interference of Waves Beats Double Slit

Physics 1B03summer-Lecture 10

QuizQuiz

Why do we see many colours on a soap bubble?

A) because white light is made up of different wavelengths

B) because the bubble has different thickness

C) both A and B

D) because the bubble is round and light reflects from the other side