Skip to content
K Knidox Search…
Physics · Waves

Doppler Effect Calculator

Find the observed frequency when a sound source or listener is moving.

Hz
Pitch emitted by the source.
m/s
343 m/s in air at 20 °C.
m/s
How fast the listener moves.
Observer direction
m/s
How fast the source moves.
Source direction
Everyday scenarios — tap to load
Observed frequency (f′)
1095.8Hz

Shift: +95.8 Hz higher — the pitch rises.

Observed frequency vs source speed (rises as it nears the speed of sound)
Observed frequency rising as the source speed increases toward the speed of sound10000 Hz1000 Hzsource 0 m/s308.7 m/s

The Doppler effect shifts the pitch you hear when a sound source or listener moves. A 1000 Hz siren approaching you at 30 m/s (with sound at 343 m/s) is heard at f′ = 1000 × 343 ÷ (343 − 30) = 1095.8 Hz — higher. It drops to about 920 Hz once the siren passes and recedes.

What the Doppler effect is

The Doppler effect is the change in a wave’s observed frequency caused by motion between the source and the observer. As a sound source moves toward you, each wavefront is emitted a little closer than the last, so the crests arrive more often and the pitch rises. As it moves away, the crests spread out and the pitch falls. The wave’s speed through the air does not change — only how often the crests reach your ear.

f′ = f · (v + vₒ) ÷ (v − vₛ)

f′ = observed frequency, f = source frequency, v = speed of sound (343 m/s in air), vₒ = observer speed (+ toward source), vₛ = source speed (+ toward observer)

Worked example

An ambulance siren emits f = 1000 Hz and drives toward a stationary listener at vₛ = 30 m/s, with the speed of sound v = 343 m/s and the observer at rest (vₒ = 0):

  1. 1
    Write the Doppler equation. f′ = f · (v + vₒ) ÷ (v − vₛ), with all speeds in m/s and frequency in Hz.
  2. 2
    Sign the speeds. Toward the other party is positive. Here vₒ = 0 (listener still) and vₛ = +30 m/s (source approaching).
  3. 3
    Substitute the values. f′ = 1000 × (343 + 0) ÷ (343 − 30) = 343000 ÷ 313.
  4. 4
    Compute the observed frequency. f′ ≈ 1095.8 Hz — about 96 Hz higher than the emitted 1000 Hz.

Sign conventions for vₒ and vₛ

Motion that shortens the gap between source and observer raises the pitch (a positive shift).

Who is movingDirectionSign in the formulaEffect on pitch
Observer (vₒ)Toward the source+vₒ (adds to numerator)Higher
Observer (vₒ)Away from the source−vₒ (subtracts)Lower
Source (vₛ)Toward the observer+vₛ (subtracts in denominator)Higher
Source (vₛ)Away from the observer−vₛ (adds in denominator)Lower

Why the pitch drops as it passes

The switch happens at the moment of passing. While the source approaches, vₛ is positive and the denominator (v − vₛ) is small, so f′ is high. The instant it goes by and starts receding, vₛ flips sign, the denominator grows, and f′ drops below the emitted frequency. That sudden fall — high to low — is the familiar “neeeow” of a passing car or siren.

Supersonic sources break the model. If the source reaches the speed of sound (vₛ = v) the denominator hits zero and the formula blows up; beyond it (vₛ > v) the source outruns its own wavefronts and a shock wave — a sonic boom — forms instead of a simple pitch shift. This everyday formula applies only when the source moves slower than sound.

Why does the pitch change when a source moves?
Motion compresses or stretches the spacing between wavefronts. Approaching, each crest is emitted nearer than the last so crests arrive more often and pitch rises; receding, they spread out and pitch falls. The sound’s speed in air is unchanged.
What are the sign conventions for vₒ and vₛ?
Speeds are positive when the motion is toward the other party. In f′ = f · (v + vₒ) ÷ (v − vₛ), a positive vₒ (observer toward source) adds to the top, and a positive vₛ (source toward observer) shrinks the bottom — both raise f′.
Why does the source term go in the denominator?
A moving source changes the wavelength emitted, which is a division by (v − vₛ), while a moving observer changes the rate crests are met, a multiplication by (v + vₒ). That is why source speed sits on the bottom and observer speed on the top.
What speed of sound should I use?
About 343 m/s in dry air at 20 °C. It rises roughly 0.6 m/s per °C, so use ~331 m/s at 0 °C. In water (~1480 m/s) or steel (~5960 m/s) use that medium’s speed instead.
What happens if the source travels at the speed of sound?
The denominator (v − vₛ) becomes zero and the formula is undefined. Physically the source keeps pace with its own wavefronts, which pile up into a shock wave — the classic sonic boom — so the simple Doppler formula no longer applies.
Does the Doppler effect work for light too?
Yes, light is Doppler-shifted (redshift and blueshift), but this calculator uses the classical sound formula. Light needs the relativistic Doppler equation because there is no medium and speeds can approach the speed of light.