Sound and Doppler Effect Flashcards

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1
Q

Speed of Sound in Solid, Liquid, and Gas

Speed of Longitudinal Wave in Gaseous Media

A
  • Sound propogates through a solid at a greater rate than a liquid and gas
    • The stronger the force between any two molecules, the greater the restoring force between those molecules
    • The faster molecules are restored, the faster they propogate, aka, faster speed
  • v = ((γRT)/(M))1/2
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2
Q

Pitch

A
  • The pitch regards the frequency of a sound
    • High pitch means higher frequency while low pitch refers to a lower frequency
  • Frequency of sound is directly proportional to pitch
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3
Q

Intensity

Intensity Formula

A
  • Intensity regards the loudness of a sound
    • Higher intensity means loud and lower intensity means soft
  • Amplitude of wave is directionaly proportional to intensity
  • Intensity = (energy)/(area x time) = (power)/(area) = P/A
    • Recall, (energy/time) = power
    • W/m2
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4
Q

Decible

A
  • We can compare the intensity of a sound with the intensity of a reference sound
  • β = (10)log(I/I0) = the intensity level, in units decible (dB)
  • Decibles measure log increases of intensity
    • So, from 0 dB to 10 dB, there has been a 10 fold increase in intensity
    • From 0 dB to 20 dB, there has been a 100 fold increase in intensity
    • From 0 dB to 30 dB, there has been a 1000 fold increase in intensity, etc.
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5
Q

Doppler Effect

A
  • There is a chnage in the intensity of the sound with distance, as well as a perceived change in the frequency (pitch) of the sound. The change in pitch of a sound from a high frequency as it approaches an observer to a low frequency as it moves way from the observer. This is called the doppler effect.
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6
Q

Doppler Effect Equation

A
  • fL = ((v + vL)/(v))fs
    • When the listener (L) moves towards a source (S), the observed frequency increases; when the L moves away from an S, the observed frequnecy decreases
  • fL = ((v)/(v - vs))fs
    • When the S moves towards the L, the observed frequency increases; when the S moves away from the L, the observed frequency decreases
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7
Q

Fundamental Frequency

A
  • The fundamental frequency is the first harmonic in a series of related waves
  • f1 = v/(2L)
  • λ1 = 2L
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8
Q

Harmonics

A
  • Harmonics refer to the frequencies that are integer multiples of the fundamental frequency, f1
  • fn = nf1
  • λn = (λn)/n
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9
Q

Open Pipes

A
  • Open pipes can vibrate at all multiples of the fundamental frequency
  • fn = (nv)/(2L)
    • f = v/(2L)
    • λ = 2L; L = λ/2
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10
Q

Closed Pipe

A
  • Closed pipes cannot vibrate at twice the fundamental frequency
  • fn = (nv)/(4L)
    • n = 1, 3, 5, …
    • f = v/(4L)
    • λ = 4L; L = λ/4
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