Skip to content

Course home

Sign up

7.2.3 The Doppler effect and red-shift

The Doppler effect

Definition

Doppler effect

The Doppler effect is the change in the observed frequency and wavelength of a wave that occurs when the source is moving relative to the observer.

Definition

Frequency

The number of complete waves or oscillations passing a point each second.

Definition

Wavelength

The distance between consecutive points on a wave that are at the same stage of an oscillation.

  1. A stationary source sends out waves as a set of evenly spaced circles, so every observer around it measures the same wavelength and the same frequency.
  2. Once the source starts to move it travels a short distance between sending out one wave and sending out the next, so each new wave leaves from a slightly different place.
  3. Ahead of the moving source the waves are squashed together, so an observer in front measures a shorter wavelength and a higher frequency.
  4. Behind the moving source the waves are stretched apart, so an observer behind measures a longer wavelength and a lower frequency.
  5. Only the relative motion of source and observer matters, so the same change is measured whether the source approaches the observer or the observer approaches the source.
  6. The source itself never changes what it emits, since the change is created entirely by the motion and appears only in what the observer receives.
  7. Wavelength and frequency shift in opposite senses because the wave speed is set by the material the wave travels through, and v=f×λv = f \times \lambdav=f×λ must still hold.

Sound from a moving source

  1. The everyday example is an ambulance siren heard from the pavement as the ambulance drives past.
  2. While the ambulance approaches, the sound waves reaching you are compressed, the frequency you hear is higher than the siren produces, and the note sounds higher pitched.
  3. The moment the ambulance passes, the waves reaching you are stretched instead, and the note drops to a lower pitch even though the siren has been set to one steady note throughout.
  4. The driver hears no change at all, because the ambulance and the siren are not moving relative to each other.
  5. The speed of sound in the air stays at about 340 m/s340\ \text{m/s}340 m/s the whole time, so a shorter wavelength has to mean a higher frequency.
  6. The faster the source travels, the larger the change in the observed frequency, which is why a passing racing car produces a far more dramatic drop than a passing bicycle bell.

Waves from a moving source bunch up in front of it and spread out behind it, which is why the observed wavelength depends on which side of the source you stand.

Light from a moving source

Definition

Red-shift

Red-shift is the increase in the observed wavelength, and decrease in the observed frequency, of light from a source that is moving away from the observer.

Definition

Blue-shift

Blue-shift is the decrease in the observed wavelength, and increase in the observed frequency, of light from a source that is moving towards the observer.

  1. Light is a wave, so a light source moving relative to an observer produces the same change in observed wavelength and frequency as a moving sound source does.
  2. A source moving away gives a longer observed wavelength and a lower observed frequency, and the light is described as red-shifted because red sits at the long wavelength end of the visible spectrum.
  3. A source moving towards the observer gives a shorter observed wavelength and a higher observed frequency, and the light is described as blue-shifted.
  4. The shift is detected by comparing the wavelengths of absorption lines from a star with the wavelengths the same elements produce in a laboratory.
  5. Everyday speeds give shifts far too small to notice, because light travels at 3.0×108 m/s3.0 \times 10^{8}\ \text{m/s}3.0×108 m/s and a car is slower than that by a factor of many millions.
  6. The size of the shift depends on how fast the source is moving along the line of sight, so a larger shift means a larger speed of approach or recession.

Absorption lines from a receding source sit at longer wavelengths than the laboratory pattern while lines from an approaching source sit at shorter wavelengths.

Example

Pitch of an approaching siren

  • A siren produces a steady note of frequency 850 Hz850\ \text{Hz}850 Hz and the speed of sound in air is 340 m/s340\ \text{m/s}340 m/s.
  • Rearranging v=f×λv = f \times \lambdav=f×λ gives λ=vf=340850=0.40 m\lambda = \dfrac{v}{f} = \dfrac{340}{850} = 0.40\ \text{m}λ=fv​=850340​=0.40 m for a stationary siren.
  • As the source drives towards a listener the waves ahead of it are compressed and the observed wavelength falls to 0.36 m0.36\ \text{m}0.36 m.
  • The speed of sound in the air is unchanged, so f=vλ=3400.36f = \dfrac{v}{\lambda} = \dfrac{340}{0.36}f=λv​=0.36340​.
  • The observed frequency is about 940 Hz940\ \text{Hz}940 Hz, which is higher than the emitted frequency and is heard as a higher pitch.
Example

A star moving towards the Earth

  • A hydrogen line has a laboratory wavelength of 486 nm486\ \text{nm}486 nm and is recorded from a star at 480 nm480\ \text{nm}480 nm.
  • The observed wavelength is shorter than the laboratory value, so the light is blue-shifted.
  • Using f=vλf = \dfrac{v}{\lambda}f=λv​ the laboratory frequency is 3.0×108486×10−9=6.17×1014 Hz\dfrac{3.0 \times 10^{8}}{486 \times 10^{-9}} = 6.17 \times 10^{14}\ \text{Hz}486×10−93.0×108​=6.17×1014 Hz.
  • The observed frequency is 3.0×108480×10−9=6.25×1014 Hz\dfrac{3.0 \times 10^{8}}{480 \times 10^{-9}} = 6.25 \times 10^{14}\ \text{Hz}480×10−93.0×108​=6.25×1014 Hz, which is higher.
  • A shorter wavelength and a higher frequency together show that the star is moving towards the Earth.
Exam technique

Describing an observed change

  • Say observed frequency and observed wavelength rather than just frequency and wavelength, because the emitted values never change.
  • Give the change in both quantities, since a mark is usually available for the wavelength and another for the frequency.
  • State the direction of motion clearly as towards or away from the observer, because approaching and receding give opposite answers.
  • Keep the wave speed constant in any calculation, and use v=f×λv = f \times \lambdav=f×λ to convert between the two observed quantities.
  • Convert nanometres to metres before substituting, since 486 nm486\ \text{nm}486 nm is 486×10−9 m486 \times 10^{-9}\ \text{m}486×10−9 m.
Common Mistake
  • Do not say that the source changes the frequency it emits, because the source is unchanged and only the observed value differs.
  • Do not say the wave travels faster when the source approaches, since the wave speed depends on the material rather than the motion of the source.
  • Do not let wavelength and frequency change in the same direction, because one rises exactly as the other falls.
  • Do not confuse loudness with pitch, because a passing siren changes pitch while its loudness changes for a different reason.
Self review
  • State what happens to the observed wavelength and frequency when a source moves towards an observer.
  • Explain why the waves ahead of a moving source are closer together.
  • Describe what the driver of an ambulance hears compared with a person on the pavement.
  • Define red-shift and blue-shift in terms of observed wavelength.
  • Calculate the observed frequency of a sound of wavelength 0.36 m0.36\ \text{m}0.36 m travelling at 340 m/s340\ \text{m/s}340 m/s.
PreviousNext

How was this guide?

Teach Genie

Review 7.2.3 The Doppler effect and red-shift by teaching Genie

Teach it back in your own words, spot gaps, and remember it better.

Start teaching
Genie and Baby Genie

7.2.3 The Doppler effect and red-shift Revision Guide

  1. GCSE
  2. /Physics
  3. /7.2.3 The Doppler effect and red-shift

Revision notes for Edexcel GCSE Physics 7.2.3 The Doppler effect and red-shift: explanations and worked examples.

Revision guides