Overview
The Doppler effect is the change in observed frequency (or wavelength) of a wave when there is relative motion between the source and observer.
Basic Concept
- When source approaches observer: frequency increases (higher pitch)
- When source moves away: frequency decreases (lower pitch)
- Same applies when observer moves toward or away from source
General Formula
f′=f×v∓vsv±vo
Where:
- f′ = observed frequency
- f = source frequency
- v = wave speed in medium
- vo = observer velocity
- vs = source velocity
Sign Convention
- Upper signs: approaching
- Lower signs: receding
- Observer moving toward source: + in numerator
- Source moving toward observer: − in denominator
Special Cases
Stationary Observer, Moving Source
Source approaching:
f′=f×v−vsv
Source receding:
f′=f×v+vsv
Stationary Source, Moving Observer
Observer approaching:
f′=f×vv+vo
Observer receding:
f′=f×vv−vo
Both Moving (Same Direction)
Source following observer:
f′=f×v−vsv−vo
Source ahead, observer behind:
f′=f×v+vsv+vo
Wavelength Changes
The observed wavelength:
λ′=f′v=λ×v±vov∓vs
For stationary observer, moving source:
λ′=λvv−vs(approaching)
λ′=λvv+vs(receding)
Doppler Effect for Light
For electromagnetic waves (where v=c):
Relativistic Formula
f′=f×c+vrelc−vrel
For v≪c (non-relativistic approximation):
f′≈f×(1−cvrel)(receding)
f′≈f×(1+cvrel)(approaching)
Redshift and Blueshift
- Redshift: Source moving away → lower frequency, longer wavelength
- Blueshift: Source approaching → higher frequency, shorter wavelength
Redshift Parameter
z=λemittedλobserved−λemitted=λΔλ
For receding source:
z=cv(for v≪c)
Shock Waves
When source moves faster than wave speed (vs>v):
Mach Number
M=vvs
Shock Wave Angle
sin(θ)=vsv=M1
- M<1: Subsonic
- M=1: Sonic (sound barrier)
- M>1: Supersonic (sonic boom)
Examples
Example 1: Car Horn
A car horn (f=400 Hz) approaches at 30 m/s. Find observed frequency (v=343 m/s).
f′=f×v−vsv=400×343−30343=400×313343=438 Hz
Example 2: Police Siren
A police car (siren at 1000 Hz) moves at 40 m/s toward a stationary observer, then passes.
Approaching:
f′=1000×343−40343=1133 Hz
Receding:
f′=1000×343+40343=896 Hz
Frequency change: 1133−896=237 Hz
Example 3: Moving Observer
A person runs at 5 m/s toward a stationary 500 Hz source.
f′=500×343343+5=507 Hz
Example 4: Both Moving
A train (500 Hz whistle) moves at 20 m/s toward a car moving at 15 m/s toward the train.
f′=500×343−20343+15=500×323358=554 Hz
Example 5: Sonic Boom
A jet flies at Mach 2.5. Find the shock wave angle.
sin(θ)=M1=2.51=0.4
θ=sin−1(0.4)=23.6°
Example 6: Galaxy Redshift
A galaxy shows hydrogen line at 680 nm (lab value: 656 nm). Find recession velocity.
z=λΔλ=656680−656=0.0366
v=zc=0.0366×3×108=1.1×107 m/s
Applications
- Radar speed guns: Police use Doppler radar to measure vehicle speed
- Medical ultrasound: Doppler imaging for blood flow
- Astronomy: Measuring stellar velocities and cosmic expansion
- Weather radar: Tracking storm movements