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Interactive Doppler effect: a moving source emits circular wavefronts that compress ahead and stretch behind. Adjust source speed to see the frequency shift.

Variables

SymbolNameSIDimensionRange
fprimef_primeObserved frequencyoutput
Frequency perceived by the observer
HzT^-11 – 2000
ffSource frequency
Frequency emitted by the source at rest
HzT^-11 – 2000
vvWave speed in medium
Speed of the wave in the medium (e.g., speed of sound in air)
m/sLT^-1100 – 1500
vov_oObserver velocity
Speed of the observer toward the source (positive = approaching)
m/sLT^-1-100 – 100
vsv_sSource velocity
Speed of the source toward the observer (positive = approaching)
m/sLT^-1-100 – 100

Deep dive

Derivation
A source emitting at frequency f produces wavefronts separated by λ = v/f. If the source moves at v_s toward the observer, each successive wavefront is emitted v_s/f closer, compressing the effective wavelength to λ' = (v - v_s)/f. The observer moving at v_o toward the source encounters wavefronts at rate f' = (v + v_o)/λ' = f·(v + v_o)/(v - v_s).
Experimental verification
Buys Ballot (1845) placed trumpeters on a train to verify pitch shifts. Modern: police radar guns use the electromagnetic Doppler effect, and Doppler ultrasound measures blood flow velocity in medical imaging.
Common misconceptions
  • The Doppler effect changes the speed of sound — it changes the observed frequency and wavelength, not the wave speed in the medium.
  • It only applies to sound — it applies to all waves, including light (redshift/blueshift of galaxies).
  • Source and observer motion are equivalent — for mechanical waves they are not: the medium defines a preferred frame. Only for light (relativistic Doppler) are they symmetric.
Real-world applications
  • Radar speed guns: police measure vehicle speed from the frequency shift of reflected microwaves.
  • Medical ultrasound: Doppler imaging measures blood flow velocity in arteries.
  • Astronomical redshift: recession velocity of galaxies reveals the expansion of the universe.
  • Weather radar: Doppler radar detects wind speed and rotation in storm cells.

Worked examples

Approaching ambulance siren

Given:
f:
700
v:
343
v_s:
30
v_o:
0
Find: f_prime
Solution

f' = f × v/(v - v_s) = 700 × 343/(343 - 30) = 700 × 343/313 = 767.1 Hz

Receding ambulance siren

Given:
f:
700
v:
343
v_s:
-30
v_o:
0
Find: f_prime
Solution

f' = 700 × 343/(343 + 30) = 700 × 343/373 = 643.7 Hz

Scenarios

What if…
  • scenario:
    What if v_s = v (source at wave speed)?
    answer:
    Denominator → 0, f' → ∞. All wavefronts pile up into a shock wave — the sonic boom at Mach 1.
  • scenario:
    What if both source and observer move toward each other?
    answer:
    Both effects compound: f' = f·(v + v_o)/(v - v_s). The frequency shift is larger than either motion alone.
  • scenario:
    What if applied to light?
    answer:
    For electromagnetic waves, use the relativistic Doppler formula: f' = f·√((1+β)/(1-β)) where β = v/c. There is no medium, so only relative velocity matters.
Limiting cases
  • condition:
    v_s → 0, v_o → 0
    result:
    f' = f
    explanation:
    No relative motion means no frequency shift.
  • condition:
    v_s → v
    result:
    f' → ∞
    explanation:
    Source at wave speed: wavefronts pile up into a sonic boom (Mach 1).
  • condition:
    v_s → -v (receding at wave speed)
    result:
    f' → f/2
    explanation:
    Source receding at wave speed halves the observed frequency.

Context

Christian Doppler · 1842

Doppler predicted the effect for light from binary stars. Buys Ballot confirmed it in 1845 using musicians on a moving train.

Hook

Why does an ambulance siren sound higher-pitched as it approaches and lower as it drives away?

An ambulance siren emits at 700 Hz, approaching at 30 m/s. Find the perceived frequency using f' = f * v/(v - v_s) with v = 343 m/s.

Dimensions:
lhs:
f' → [T⁻¹]
rhs:
f·(v + v_o)/(v - v_s) → [T⁻¹]·[LT⁻¹]/[LT⁻¹] = [T⁻¹]
check:
Both sides are [T⁻¹] = Hz. ✓
Validity: Valid for mechanical waves when source speed < wave speed (subsonic). For electromagnetic waves, use the relativistic Doppler formula instead.

Related formulas