Sound and Doppler Effect Flashcards
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
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
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
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.
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.
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
7
Q
Fundamental Frequency
A
- The fundamental frequency is the first harmonic in a series of related waves
- f1 = v/(2L)
- λ1 = 2L
8
Q
Harmonics
A
- Harmonics refer to the frequencies that are integer multiples of the fundamental frequency, f1
- fn = nf1
- λn = (λn)/n
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
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