f' = f·c/(c−v)
An approaching source compresses wavelength in the direction of travel, so a stationary observer perceives a higher frequency than was emitted.
An approaching source compresses wavelength in the direction of travel, so a stationary observer perceives a higher frequency than was emitted.
Select a target and calculate.
An approaching source compresses wavelength in the direction of travel, so a stationary observer perceives a higher frequency than was emitted.
f=1,000 Hz, c=343 m/s and v=30 m/s give f'=1,000·343/313≈1,095.85 Hz.
Stationary observer and source moving directly toward the observer along the line of sight; medium motion (wind), oblique motion directions and the stationary-source/moving-observer case are excluded.
This calculator determines the frequency arriving at a stationary observer from an approaching sound source, the physical principle behind the familiar pitch rise of an approaching vehicle.
A source approaching the observer at speed v compresses the emitted waves in the direction of travel. The stationary observer perceives the higher frequency f'=f·c/(c−v).
f' = f·c/(c−v)
f' = f·c/(c−v)| Symbol / input | Meaning |
|---|---|
| Perceived frequency f' | Frequency arriving at the stationary observer. |
| Emitted frequency f | Frequency emitted by the moving source. |
| Speed of sound c | Propagation speed of sound in the medium. |
| Source speed v | Speed of the source approaching the observer; must be less than c. |
f is the frequency emitted by the source, c the speed of sound in the medium, v the speed of the approaching source.
Take f from the known emitted frequency, derive c from air temperature, and v from the source's approach speed.
f=1,000 Hz, c=343 m/s and v=30 m/s give f'=1,000·343/313≈1,095.85 Hz.
The closer v approaches c, the more strongly perceived frequency rises; at v=c the denominator would reach zero and the formula diverges (the sonic-boom limiting case).
f and f' are frequencies, c and v are speeds.
Explaining and calculating the Doppler effect for sirens and passing vehicles and in teaching; a basis for Doppler radar and ultrasonic measurements.
Stationary observer and a source moving exactly along the line of sight directly toward the observer; oblique motion directions (needing a cosine correction), wind effects on c, and the case of a moving observer with a stationary source are excluded.
Common mistake: Do not enter v≥c; the formula holds only for subsonic source speeds and otherwise gives no physically meaningful result.
Explaining and calculating the Doppler effect for sirens and passing vehicles and in teaching; a basis for Doppler radar and ultrasonic measurements.
f is the frequency emitted by the source, c the speed of sound in the medium, v the speed of the approaching source.
Stationary observer and a source moving exactly along the line of sight directly toward the observer; oblique motion directions (needing a cosine correction), wind effects on c, and the case of a moving observer with a stationary source are excluded.