<p align="right">Last Update: <font color="#4f81bd">January 02, 2025</font></p>
## BIG IDEAS
- The Doppler effect is a change in the observed pitch of a sound or light, due to **relative motion** between the source and the observer.
- Pointed out by [[Johann Christian Doppler]] in 1842.
- Tested in 1845 by Christopher Heinrich Dietrich Buys-Ballot.
- Determine velocities of solar prominences, double stars, rings of Saturn.
- Used to determine distances of nearby stars.
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### Textbook Alignment
Walker 14-6 Doppler Effect
Consider an ambulance, fire truck, or police vehicle with a siren blaring as it is moving toward you then passing you.
- The [[Frequency|frequency]] is higher when the vehicle is moving toward you.
- The [[Wavelength|wavelength]] is shorter (compression)
- The frequency is lower as the vehicle moves away from you.
- The wavelengths are low pressure (rarefaction).
- This effect is known as the Doppler effect.
![[Doppler.png]]
### Moving Source
For a stationary observer and a <font color="#f79646">moving sound source</font>, the perceived frequency ( $f_{obs}$ ) is
$f_{obs} = f_s( \frac{v_w}{v_w \pm v_s}) \tag{1}$
Where:
$f_s$ is the sound from a source,
$v_s$ is the speed of the source,
$v_w$ is the speed of sound.
Use a minus sign for motion toward the observer and a plus sign for motion away from the observer.
### Stationary Source
For a moving observer and a <font color="#f79646">stationary sound source</font>, the perceived frequency ( $f_{obs}$ ) is
$f_{obs} = f_s (\frac{v_w \pm v_{obs}}{v_w})$
Where:
$v_{obs}$ is the velocity of the observer.
Use a plus sign for motion toward the source and a negative sign for motion away from the source.
### Slide Deck
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### Related Topics
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[[Home|Home]] | [[Oscillations]] | [[Waves]] | [[Module 0 Sound]] | [[Module 1 Sound Waves]] | [[Module 2 Speed of Sound]] | [[Module 3 Sound Intensity]] | [[Module 4 Doppler Effect]] | [[Electromagnetic radiation]]