Interference and Doppler Effect Flashcards

1
Q

Interference of Travelling Waves
2 harmonic waves, equal amplitude and frequency
Description of Resultant Wave

A

-resulting wave from the superposition of these two waves is also a harmonic travelling wave with the same frequency and wavelength as the two original waves

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2
Q

Interference of Travelling Waves
2 harmonic waves, equal amplitude and frequency
Equation

A

resulting wave function:
y = 2A cos(Φ/2) sin(kx-ωt+Φ)

amplitude = 2A cos(Φ/2)
where A = amplitude of original waves and Φ = phase difference

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3
Q

Interference of Travelling Waves
2 harmonic waves, equal amplitude and frequency
Constructive Interference

A

Φ = 0 or any even multiple of π

the two waves are in phase and interfere constructively

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4
Q

Interference of Travelling Waves
2 harmonic waves, equal amplitude and frequency
Destructive Interference

A

Φ = any odd multiple of π

the two waves are in antiphase and interfere destructively

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5
Q

Waves From Two Sources

Pressure Equation

A
Wave 1 is a distance r1 from ear:
P1 = P0 sin (k*r1 - ωt)
Wave 2 is a distance r2 from ear:
P2 = P0 sin k*r2 - ωt)
Pressure at Ear
P = P1 + P2 = P0 [ sin (k*r1 - ωt) + sin k*r2 - ωt)]
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6
Q

Waves From Two Sources

Phase Difference

A

Φ = kr1 - kr2 = 2πΔ / λ

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7
Q

Waves From Two Sources

Path Difference

A

Δ = r1 - r2

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8
Q

Constructive Interference

Definition

A

maximum sound heard when path difference is 0 or an integral number of wavelengths

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9
Q

Destructive Interference

Definition

A

non sound is hears, occurs when path difference is a half integral number of wavelengths

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10
Q

Coherent

Definition

A

two sound sources are coherent if their phase distance is consistent, i.e. not random

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11
Q

When do beats occur?

A

-occurs when 2 harmonic waves have slightly different frequency

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12
Q

Beats

Equation

A
y = y1 + y2
y = 2A cos [2πt((f1-f2)/2)] cos[2πt((f1+f2)/2)]
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13
Q

Beats

Equation Explained

A

y = 2A cos [2πt((f1-f2)/2)] cos[2πt((f1+f2)/2)]

Slow Amplitude Modulation, frequency of change in amplitude = f1-f2 / 2
Rapidly oscillating carrier wave, frequency of resultant wave = f1+f2 / 2

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14
Q

When is a beat heard?

A

-when amplitude is maximum or minimum, twice every cycle (at frequency of amplitude modulation)

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15
Q

Intensity of Two Incoherent Sources

A

-sources are incoherent so there is no interference
-intensity is isotropic
I = I1 + I2

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16
Q

Doppler Effect

Observer Moving Towards Stationary Source

A

-observer detects more wavefront per unit time

f’ = f ((v+v0)/v)

f' = perceived frequency
f = actual frequency
v = wave speed
v0 = speed of observer
17
Q

Doppler Effect

Observer Moving Away From Stationary Source

A

-observer detects fewer wave fronts per unit time

f’ = f((v-v0)/v)

f' = perceived frequency
f = actual frequency
v = wave speed
v0 = speed of observer
18
Q

Doppler Effect

Source Moving Towards Stationary Observer

A

-wave length is shortened, wave fronts are closer together

f’ = f(v/(v-vs))

f' = perceived frequency
f = actual frequency
v = wave speed
vs = source velocity
19
Q

Doppler Effect

Source Moving Away From Stationary Observer

A

-wave fronts are further apart as wavelength is greater

f’ = f (v/(v+vs))

f' = perceived frequency
f = actual frequency
v = wave speed
vs = source velocity
20
Q

Doppler Effect

Source and Observer in Motion

A

f’ = f [ (v±v0) / (v∓vs)

(upper sign for towards, lower sign for away from)

f' = perceived frequency 
f = actual frequency
v = wave speed
v0 = observer speed 
vs = source speed
21
Q

Shock Waves

A
  • occur when the speed of the source approaches the speed of sound
  • the source travels a distance vs*t in time t
  • but in that time the wavefront emitted at time t=0 has also travelled the same distance
  • this creates a conical shock front
22
Q

Intensity of Two Coherent Sources In Phase

A

It = (√I1 + √I2)²

23
Q

Intensity of Two Coherent Sources Out of Phase

A

It = (√I1 - √I2)²