Standing Waves Flashcards

1
Q

Wave Function for Standing Waves

A

y == 2A0 sin(kx) cos(ωt)

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2
Q

Standing Waves

Description

A
  • every part of the string vibrates with SHM with the same frequency and phase
  • amplitude is dependent on x
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3
Q

Standing Waves on a String

A
  • natural patterns of oscillation of the string each with a different characteristic frequency
  • the length of the string is always equal to an integer number of half wavelengths
  • fundamental has the longest wavelength, λ/2=L
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4
Q

Harmonics and Overtones

A
  • the fundamental is the lowest frequency mode
  • frequency of each normal mode is an integer multiple of the fundamental frequency
  • these integer multiples are called harmonics
  • the fundamental is the first harmonic and so on
  • these normal mode frequencies are also referred to as overtones, where the 2nd harmonic is the first over tone, the 3rd harmonic is the 2nd overtone so on
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5
Q

Standing Waves on a String

Description

A

when a stretched string is distorted so that the initial shape corresponds to a harmonic, only that particular normal mode is excited, so the string vibrates with the frequency of that harmonic

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6
Q

Standing Waves – Musical Instruments

Description

A

-when a string is struck/plucked on a piano/guitar, its initial shape is no that of a single normal mode. Several normal modes are excited resulting in vibration that includes several harmonic frequencies. Typically, the fundamental has the largest amplitude

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7
Q

Sound Waves

A
  • longitudinal
  • move through gases, liquids or solids
  • speed depends on the properties of the medium
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8
Q

Classifying Sound Waves

A

Audible Waves - 20-20000 Hz
Infrasonic Waves - frequency below audible
Ultrasonic Waves - frequency higher than audible

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9
Q

Energy of a Sound Wave

A

Etot = 1/2 ρ(ωs0)² A vt

s0 = amplitude of sound wave
A = surface area
v = speed of wave
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10
Q

Sound Wave - Wave FUnction

A

S = S0 cos(ωt)

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11
Q

Maximum Velocity of a Sound Wave

A

Vmax = ωS0

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12
Q

Energy Density of a Sound Wave

A

1/2 ρω²S0²

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13
Q

Power

Definition (Sound Wave)

A

rate at which energy is transmitted to each layer

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14
Q

Power of a Sound Wave

A

P = 1/2 ρ(ωs0)² A v

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15
Q

Intensity of a Sound Wave

A

I = 1/2 ρ(ωs0)² v

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16
Q

Standing Waves in Air Columns

Open at Both Ends

A
  • nodes at each end of the tube
  • first normal mode, L = λ/2
  • second normal mode, L = λ
  • third normal mode, L = 3λ/2
  • the integer numbers of half wavelengths of the normal modes are equal to the length
17
Q

Standing Waves in Air Columns

Open at One End

A
  • antinode at the closed end
  • node at the open end
  • first normal mode, L = λ/4
  • second normal mode, L = 3λ/4
  • third normal mode, L = 5λ/4
  • for the normal modes L is equal to odd integer numbers of quarter wavelengths
18
Q

Pressure Wave

Velocity Equation

A

v = √(B/p)

B = bulk modulus of compressibility
p = density 
v = velocity
19
Q

Bulk Modulus of Compressibility

Equation

A

B = γp

γ = Cp/Cv

20
Q

Pressure Wave Equation

A

ΔP = BkS0 cos(kx-ωt)

21
Q

Amplitude of Sound Wave

Pressure Equation

A

S0 = ΔP0 / ρωv

22
Q

Sound Wave Intensity

Pressure Equation

A

I = 1/2 ρω²v {ΔP0/ρωv}²

23
Q

Spherical Waves

A
  • in a uniform medium, waves move outwards from the source at constant speed
  • from a point source (a small object oscillating with SHM) are produced with spherical wavelengths
24
Q

Intensity and Amplitude

A

I ∝ A²

-> I = cA²
A = √(I/c)

c = constant of proportionality

25
Q

Decibels

A

-a lotharithmic scale

β = 10 log(10){I/I0)

β = measured in decibels (dB)
I = Intensity of the sound
I0 = threshold of hearing