Doppler Effect

Site: Young Education
Cours: Waves
Livre: Doppler Effect
Imprimé par: Guest user
Date: lundi 9 novembre 2026, 16:36

1. Relative Motion and Frequency

Learning outcomes
  • I can describe relative motion between a source and an observer.
  • I can explain observed changes in frequency.
  • I can distinguish between emitted and observed frequency.
  • I can predict when frequency increases or decreases.
  • I can describe everyday examples of the Doppler effect.

Relative Motion and Frequency

When a wave source and an observer move relative to one another, the observer may detect a frequency that is different from the frequency produced by the source. This phenomenon is called the Doppler effect.

The Doppler effect occurs with many types of waves, including:

  • sound waves
  • water waves
  • light and other electromagnetic waves

A familiar example is the changing pitch of a siren as an emergency vehicle approaches and then passes an observer.

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6

Relative Motion

Relative motion describes the motion of one object compared with another object.

For the Doppler effect, the two important objects are:

  • the source of the waves
  • the observer detecting the waves

The source might be:

  • an ambulance siren
  • a car horn
  • a train whistle
  • a loudspeaker
  • a star producing light

The observer might be:

  • a person
  • a microphone
  • a radar detector
  • an ultrasound transducer
  • a telescope

What matters is how the distance between the source and observer changes.


Approaching and Receding

There are two basic situations.

Approaching

The distance between the source and observer is decreasing.

Receding

The distance between the source and observer is increasing.

The Doppler effect depends on this relative motion.

A useful rule is:

approaching → observed frequency increases

receding → observed frequency decreases


The Doppler Effect

The Doppler effect is the observed change in frequency caused by relative motion between a wave source and an observer.

The source continues producing waves at its own frequency.

However, relative motion changes the rate at which wavefronts reach the observer.

Therefore, the observer can detect a different frequency.


Emitted Frequency

The emitted frequency is the frequency actually produced by the source.

It may be written as:

fₛ

where the subscript s represents the source.

For example, suppose an ambulance siren produces:

fₛ = 800 Hz

The siren continues producing approximately 800 cycles each second regardless of whether the ambulance is approaching or receding from a stationary observer.


Observed Frequency

The observed frequency is the frequency detected by the observer.

It may be written as:

fₒ

where the subscript o represents the observer.

Because of relative motion:

fₒ does not necessarily equal fₛ

For an approaching source:

fₒ > fₛ

For a receding source:

fₒ < fₛ

If there is no relevant relative motion:

fₒ = fₛ


Emitted vs Observed Frequency

Situation Emitted Frequency Observed Frequency
No relative motion fₛ fₒ = fₛ
Approaching fₛ fₒ > fₛ
Receding fₛ fₒ < fₛ

The source frequency does not have to change for the observer to hear or detect a frequency change.

This distinction is central to understanding the Doppler effect.


A Moving Sound Source

Imagine a stationary siren producing sound waves.

If the siren is not moving, its wavefronts spread outward with equal spacing in every direction in still air.

Now suppose the siren begins moving forward.

Between producing one wavefront and the next, the siren changes position.

As a result:

  • wavefronts become closer together in front
  • wavefronts become farther apart behind

This changes the wavelength reaching observers.

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Source Moving Toward the Observer

Suppose a source moves toward a stationary observer.

Each new wavefront is emitted from a position slightly closer to the observer than the previous wavefront.

The wavefronts in front of the source become:

compressed

Therefore, the wavelength in front of the moving source becomes shorter.

Since:

v = fλ

and the speed of sound through the same stationary medium remains approximately constant:

shorter wavelength → higher observed frequency

The observer therefore detects a higher frequency.


Approaching Source

The sequence is:

source approaches

→ wavefronts become closer together

→ wavelength decreases

→ wavefronts arrive more frequently

→ observed frequency increases

For sound:

higher observed frequency → higher perceived pitch


Source Moving Away from the Observer

Now suppose the source moves away from the observer.

Each new wavefront is produced from a position farther away.

The wavefronts behind the moving source become:

more widely spaced

Therefore:

wavelength increases

With approximately constant wave speed:

longer wavelength → lower observed frequency

The observer detects a lower frequency.


Receding Source

The sequence is:

source recedes

→ wavefronts spread farther apart

→ wavelength increases

→ wavefronts arrive less frequently

→ observed frequency decreases

For sound:

lower observed frequency → lower perceived pitch


The Ambulance Example

An ambulance siren provides one of the most familiar examples of the Doppler effect.

As the ambulance approaches:

  • wavefronts are compressed
  • observed wavelength is shorter
  • observed frequency is higher
  • the siren sounds higher in pitch

As the ambulance moves away:

  • wavefronts are farther apart
  • observed wavelength is longer
  • observed frequency is lower
  • the siren sounds lower in pitch
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What Happens as the Vehicle Passes?

Suppose you stand beside a road while an emergency vehicle approaches and passes.

Before it reaches you:

observed frequency > emitted frequency

After it passes:

observed frequency < emitted frequency

You therefore hear a noticeable drop in pitch around the time the vehicle passes.

The siren itself has not suddenly changed its emitted frequency.

The relative motion has changed.


Pitch and Frequency

For sound, pitch is our perception associated strongly with frequency.

Generally:

higher frequency → higher pitch

lower frequency → lower pitch

Therefore, the Doppler effect for sound is often noticed as a change in pitch.

Frequency is a physical quantity measured in hertz.

Pitch is a perception produced by the auditory system.

They are closely related but are not exactly the same concept.


The Wave Speed Does Not Increase Because the Source Moves

A common misconception is that sound travels faster in front of a moving vehicle because the vehicle is moving forward.

For ordinary sound waves in still air, this is incorrect.

The speed of sound is determined mainly by the properties of the medium.

The moving source changes the:

spacing between wavefronts

It does not simply add its speed to the speed of sound through the air.


Wave Speed, Frequency, and Wavelength

The wave equation is:

v = fλ

For sound travelling through the same region of air, v remains approximately constant.

If the source approaches:

λ decreases

so the observer encounters wavefronts more frequently.

If the source recedes:

λ increases

so the observer encounters wavefronts less frequently.

This produces the Doppler shift in observed frequency.


Example: Wavefront Spacing

Suppose a stationary siren produces sound with:

f = 500 Hz

and sound speed is:

v = 340 m/s

The wavelength is:

λ = v/f

λ = 340/500

λ = 0.68 m

If the source moves toward an observer, the wavefronts in front become closer than 0.68 m apart.

The observer therefore detects a frequency greater than 500 Hz.

Behind the source, the wavefronts are farther apart than 0.68 m, producing an observed frequency below 500 Hz.


A Stationary Source and Moving Observer

The source does not have to move.

Suppose the source is stationary while the observer moves toward it.

The observer encounters wavefronts more rapidly.

Therefore:

observer approaches source → observed frequency increases

If the observer moves away:

observer recedes from source → observed frequency decreases

The underlying principle is still relative motion between the source and observer.


Moving Source vs Moving Observer

Both situations can produce a Doppler effect, but their physical explanations differ slightly.

Moving source

Changes the spacing of wavefronts in the medium.

Moving observer

Does not change the wavelength already present in the medium but changes how rapidly the observer encounters those wavefronts.

In both cases:

approaching → higher observed frequency

receding → lower observed frequency


Both Source and Observer Moving

The source and observer can both move.

The important question remains:

Is the distance between them increasing or decreasing?

If they move toward one another:

observed frequency increases

If they move apart:

observed frequency decreases

Their individual velocities determine the size of the frequency change.


Motion Sideways to the Observer

Suppose a source moves sideways rather than directly toward or away from an observer.

Only the component of relative velocity along the line joining the source and observer produces the ordinary Doppler shift.

This component is called the:

radial velocity

Therefore, the Doppler effect tells us primarily about motion:

toward or away from the observer

rather than motion entirely sideways across the observer's view.


Predicting Frequency Changes

A simple prediction method is:

Step 1: Identify the source.

Step 2: Identify the observer.

Step 3: Ask whether the distance between them is decreasing or increasing.

If distance decreases:

approaching → higher observed frequency

If distance increases:

receding → lower observed frequency

If their separation is momentarily not changing:

no instantaneous Doppler shift from radial motion


Doppler Effect Equation for a Moving Source

For a stationary observer and a sound source moving directly toward or away from the observer, a useful equation is:

fₒ = fₛv/(v ∓ vₛ)

where:

fₒ = observed frequency

fₛ = emitted frequency

v = speed of sound

vₛ = speed of source

For an approaching source, the denominator becomes smaller:

fₒ = fₛv/(v − vₛ)

Therefore:

fₒ increases

For a receding source:

fₒ = fₛv/(v + vₛ)

Therefore:

fₒ decreases


Worked Example: Approaching Ambulance

An ambulance siren emits:

fₛ = 700 Hz

The ambulance approaches at:

vₛ = 20 m/s

Assume:

v = 340 m/s

Use:

fₒ = fₛv/(v − vₛ)

fₒ = 700 × 340/(340 − 20)

fₒ = 238000/320

fₒ ≈ 744 Hz

The observer hears approximately:

744 Hz

This is higher than the emitted frequency of 700 Hz.


Worked Example: Receding Ambulance

The same ambulance moves away at:

20 m/s.

Use:

fₒ = fₛv/(v + vₛ)

fₒ = 700 × 340/(340 + 20)

fₒ = 238000/360

fₒ ≈ 661 Hz

The observer hears approximately:

661 Hz

So:

approaching → 744 Hz

emitted → 700 Hz

receding → 661 Hz


Doppler Effect Equation for a Moving Observer

For a stationary source and an observer moving directly toward or away from it:

fₒ = fₛ(v ± vₒ)/v

where:

vₒ = observer speed

For an observer moving toward the source:

fₒ = fₛ(v + vₒ)/v

For an observer moving away:

fₒ = fₛ(v − vₒ)/v

The signs are chosen so that approaching motion increases the observed frequency and receding motion decreases it.


Worked Example: Moving Observer

A stationary source produces:

fₛ = 600 Hz

An observer moves toward the source at:

vₒ = 10 m/s

Assume:

v = 340 m/s

Then:

fₒ = 600(340 + 10)/340

fₒ = 600 × 350/340

fₒ ≈ 618 Hz

The observer detects a higher frequency because they are moving toward the source.


The Size of the Doppler Shift

The Doppler shift is the difference between observed and emitted frequency:

Δf = fₒ − fₛ

For the approaching ambulance:

fₒ = 744 Hz

fₛ = 700 Hz

Therefore:

Δf = 744 − 700

Δf = +44 Hz

A positive shift indicates an increase in observed frequency under this convention.

For a receding source, Δf would be negative.


Faster Relative Motion Produces a Larger Shift

In general, greater speed toward or away from the observer produces a larger Doppler shift.

For example, a slowly moving bicycle bell produces only a small change.

A rapidly moving racing vehicle can produce a much more noticeable change.

Therefore:

greater radial relative speed → larger frequency shift


Everyday Examples of the Doppler Effect

Common examples include:

  • ambulance sirens
  • police sirens
  • fire-engine sirens
  • train whistles
  • car horns
  • motorcycles
  • racing vehicles
  • aircraft sounds

In each case, the observed pitch changes as the source approaches and recedes.


Train Whistle Example

Imagine standing beside a railway line.

As a train approaches:

pitch sounds higher

As it passes:

pitch drops

As it moves away:

pitch sounds lower

The train whistle does not need to change its emitted frequency.

The change results from relative motion.


Racing Vehicles

The Doppler effect is often noticeable when high-speed vehicles pass a stationary observer.

As the vehicle approaches, its engine sound contains frequencies shifted upward.

After passing, those frequencies are shifted downward.

This produces the characteristic:

high → sudden drop → lower

sound heard during a pass.


Doppler Ultrasound

The Doppler effect has important medical applications.

Doppler ultrasound uses reflected ultrasound to study moving structures, especially blood.

Ultrasound is transmitted into the body.

The waves reflect from moving blood cells.

Motion changes the frequency of the reflected ultrasound.

By measuring this frequency shift, medical equipment can obtain information about blood flow.

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Doppler Ultrasound Applications

Doppler ultrasound can help investigate:

  • blood-flow direction
  • blood-flow speed
  • heart function
  • blood vessels
  • circulation

If blood moves toward the transducer, the reflected frequency shifts one way.

If blood moves away, it shifts the opposite way.

The equipment converts these frequency changes into useful medical information.


Radar and the Doppler Effect

Radar systems can also use Doppler shifts.

Electromagnetic waves are transmitted toward a moving object.

The waves reflect from the object and return to the detector.

If the object is moving relative to the radar system, the reflected frequency is shifted.

This can provide information about the object's:

radial velocity

Applications include:

  • vehicle-speed measurement
  • aircraft tracking
  • weather radar
  • navigation

Doppler Weather Radar

Weather radar can detect electromagnetic waves reflected by precipitation.

The Doppler shift provides information about motion toward or away from the radar.

Meteorologists can use this to investigate:

  • wind motion
  • storm rotation
  • precipitation movement

This makes the Doppler effect important for weather monitoring and forecasting.


Astronomy and the Doppler Effect

The Doppler effect also applies to electromagnetic waves such as light.

Astronomers compare wavelengths observed from astronomical objects with known wavelengths produced by atoms.

Motion along the line of sight can shift the observed wavelengths.

If an object is moving away, its light can be shifted toward longer wavelengths.

This is called:

redshift

If an object is moving toward us, its light can be shifted toward shorter wavelengths.

This is called:

blueshift

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Redshift

For visible light:

longer wavelength → toward red end of spectrum

Therefore, an object moving away can produce a Doppler shift toward longer wavelengths.

This is called:

redshift

Redshift does not necessarily mean that an object literally looks red.

Scientists often measure the shift of identifiable spectral lines.


Blueshift

An object moving toward an observer produces a shift toward shorter wavelengths.

For visible light, this is toward the blue end of the spectrum.

Therefore:

approaching astronomical object → blueshift

Again, astronomers usually measure changes in spectral lines rather than simply judging the object's apparent colour.


Measuring Stellar Motion

Suppose astronomers know the normal wavelength of a particular spectral line.

They measure the same line in light from a star.

If the observed wavelength is longer:

the star has a radial component of motion away

If the wavelength is shorter:

the star has a radial component of motion toward

The size of the shift provides information about radial speed.


Detecting Exoplanets

The Doppler effect can even help detect planets orbiting other stars.

A planet and star orbit their common centre of mass.

The star therefore moves slightly:

  • toward Earth
  • then away from Earth
  • then toward Earth again

This produces small periodic shifts in the star's spectral lines.

Astronomers can analyze these changes to infer the presence of an orbiting planet.

This method is called the:

radial velocity method


Doppler Effect for Water Waves

The Doppler effect can also be observed with water waves.

A stationary source produces evenly spaced circular wavefronts.

If the source moves:

  • wavefronts become closer together ahead of it
  • wavefronts become farther apart behind it

The same basic pattern appears as for a moving sound source.

This makes water waves useful for visually demonstrating the Doppler effect.


Wavefront Diagrams

A Doppler-effect diagram often shows a moving source surrounded by wavefronts.

Look at the spacing.

Closer wavefronts

indicate shorter wavelength and higher observed frequency.

Wider-spaced wavefronts

indicate longer wavelength and lower observed frequency.

The direction in which the source is moving usually has compressed wavefronts ahead of it.


Interpreting a Doppler Diagram

Suppose a moving source travels to the right.

Wavefronts are compressed on the right.

Wavefronts are spread out on the left.

Therefore:

Observer on right:

source approaching → higher frequency

Observer on left:

source receding → lower frequency

The emitted frequency is the same source frequency for both observers.

Their observed frequencies are different.


The Observer Does Not Need to Hear the Source

The term observer does not necessarily mean a person.

An observer can be any detector.

Examples include:

  • microphone
  • ultrasound transducer
  • radar receiver
  • radio antenna
  • telescope
  • scientific sensor

Therefore, the Doppler effect is much broader than changes in audible pitch.


Doppler Effect vs Changing Source Frequency

Suppose a driver presses a control that actually changes the frequency produced by a siren.

That is:

a change in emitted frequency

It is not, by itself, a Doppler effect.

The Doppler effect occurs when relative motion causes:

observed frequency ≠ emitted frequency

Distinguishing these two situations is essential.


Doppler Effect vs Changing Loudness

As a vehicle approaches, its sound often becomes louder.

As it moves away, it often becomes quieter.

This change in loudness is mainly related to:

  • distance
  • intensity
  • spreading of sound energy

The change in pitch is related to:

Doppler frequency shift

Therefore:

loudness change ≠ Doppler effect

although both can happen simultaneously.


Doppler Effect vs Wave Speed

The Doppler effect does not mean the source has changed the normal wave speed through the medium.

For sound:

  • source motion changes wavefront spacing
  • observer motion changes encounter rate
  • the medium determines the propagation speed

For electromagnetic waves, the physics is more advanced and ultimately requires relativity for precise treatment at high speeds.


A Complete Everyday Example

An ambulance produces a siren at a constant emitted frequency.

It approaches a pedestrian.

The distance between ambulance and pedestrian decreases.

The wavefronts arriving from the approaching moving source are closer together.

The pedestrian detects:

higher observed frequency

The ambulance passes.

It now moves away.

Wavefronts reaching the pedestrian are farther apart.

The pedestrian detects:

lower observed frequency

The emitted frequency of the siren has remained essentially unchanged.

The change is caused by:

relative motion


A Complete Technology Example

A Doppler radar system transmits electromagnetic waves toward a moving vehicle.

The waves reflect from the vehicle.

Because the vehicle is moving, the reflected waves return with a shifted frequency.

The radar compares:

transmitted frequency

with:

received frequency

The frequency difference provides information about:

radial speed

The Doppler effect has therefore converted motion into a measurable frequency shift.


A Reliable Strategy for Doppler Questions

  1. Identify the source.
  2. Identify the observer or detector.
  3. Identify the emitted frequency.
  4. Determine whether the distance between source and observer is decreasing or increasing.
  5. If decreasing, predict a higher observed frequency.
  6. If increasing, predict a lower observed frequency.
  7. Distinguish emitted frequency from observed frequency.
  8. If a moving source is involved, consider wavefront compression or spreading.
  9. If a moving observer is involved, consider how rapidly the observer encounters wavefronts.
  10. Use the appropriate Doppler equation if a numerical calculation is required.
  11. Check whether your calculated result matches your prediction.
  12. For sound, relate higher frequency to higher pitch and lower frequency to lower pitch.
  13. Do not confuse frequency shift with changes in loudness.
  14. For light, connect longer wavelength with redshift and shorter wavelength with blueshift.
  15. Interpret the result in terms of relative motion.

Common Mistakes

Thinking the emitted frequency changes when the source moves

The source can continue emitting the same frequency while observers detect different frequencies.

Confusing emitted and observed frequency

Emitted frequency belongs to the source. Observed frequency is what the detector measures.

Thinking approaching means lower frequency

Approaching produces a higher observed frequency.

Thinking receding means higher frequency

Receding produces a lower observed frequency.

Thinking the sound travels faster in front of a moving vehicle

In still air, the source's motion changes wavefront spacing rather than simply increasing sound speed.

Confusing pitch and loudness

Pitch is strongly related to frequency. Loudness is related to sound intensity and human perception.

Thinking a louder approaching siren proves the Doppler effect

The Doppler effect specifically concerns the frequency shift.

Thinking only the source can move

A moving observer can also experience a Doppler shift.

Thinking any motion produces the same Doppler effect

Motion toward or away from the observer—the radial component—is what matters most.

Thinking redshift means a star simply looks red

Redshift is measured as a shift of wavelengths or spectral features toward longer wavelengths.

Thinking the Doppler effect applies only to sound

It also occurs with electromagnetic and other waves.


Key Terms

Relative motion — motion of one object compared with another.

Source — object or system producing waves.

Observer — person or detector receiving waves.

Doppler effect — observed frequency change caused by relative motion between source and observer.

Emitted frequency (fₛ) — frequency produced by the source.

Observed frequency (fₒ) — frequency detected by the observer.

Doppler shift — difference between observed and emitted frequency.

Approaching — relative motion that decreases the distance between source and observer.

Receding — relative motion that increases the distance between source and observer.

Wavefront — line or surface joining points of a wave in the same phase.

Wavelength (λ) — distance between corresponding points on consecutive waves.

Frequency (f) — number of wave cycles passing a point each second.

Pitch — auditory perception strongly associated with sound frequency.

Radial velocity — component of velocity toward or away from an observer.

Redshift — shift toward longer wavelengths, commonly associated with a receding astronomical source.

Blueshift — shift toward shorter wavelengths, commonly associated with an approaching astronomical source.

Doppler ultrasound — medical technique using frequency shifts of reflected ultrasound to investigate motion such as blood flow.

Doppler radar — radar technique using frequency shifts to determine radial motion.

Spectral line — particular wavelength associated with emission or absorption by atoms or molecules.


Key Takeaways

  • Relative motion describes motion between a source and an observer.
  • The Doppler effect is an observed change in frequency caused by relative motion.
  • Emitted frequency and observed frequency are different quantities.
  • The source can emit a constant frequency while an observer detects a changing frequency.
  • When source and observer approach each other, observed frequency increases.
  • When source and observer move apart, observed frequency decreases.
  • For sound, higher observed frequency is associated with higher perceived pitch.
  • Lower observed frequency is associated with lower perceived pitch.
  • A moving source compresses wavefronts ahead of it and spreads wavefronts behind it.
  • The wave speed through a stationary medium does not simply increase because the source moves.
  • A moving observer can also experience a Doppler shift.
  • The size of the Doppler shift increases with radial relative speed.
  • Motion perpendicular to the line of sight does not produce the ordinary instantaneous radial Doppler shift.
  • Ambulance sirens, train whistles, car horns, and racing vehicles provide everyday examples.
  • Doppler ultrasound uses frequency shifts to investigate blood flow.
  • Doppler radar can measure radial motion.
  • Weather radar uses Doppler information to investigate motion within storms.
  • Light from approaching astronomical objects can be blueshifted.
  • Light from receding astronomical objects can be redshifted.
  • Astronomers use Doppler shifts to measure stellar motion.
  • Periodic Doppler shifts can help reveal planets orbiting other stars.
  • Changes in loudness should not be confused with Doppler frequency shifts.
  • The Doppler effect provides a powerful method for measuring motion using waves.

Check Your Understanding

  1. Define relative motion between a source and an observer.
  2. Explain the Doppler effect in your own words.
  3. Distinguish between emitted frequency and observed frequency.
  4. An ambulance approaches a stationary observer while emitting a constant-frequency siren. Predict how the observed frequency compares with the emitted frequency.
  5. The same ambulance passes the observer and moves away. Predict what happens to the observed frequency and pitch.
  6. Explain why wavefronts become closer together in front of a moving sound source.
  7. Explain why the speed of sound does not simply increase because the source moves toward an observer.
  8. A stationary siren produces a frequency of 600 Hz. A moving observer travels toward it. Will the observer detect a frequency greater than, equal to, or less than 600 Hz? Explain.
  9. An ambulance emits a 700 Hz siren and approaches at 20 m/s. Using a sound speed of 340 m/s, calculate the observed frequency for a stationary observer.
  10. Calculate the observed frequency when the same 700 Hz ambulance moves away at 20 m/s.
  11. Explain why an approaching siren can become both louder and higher in pitch, but only one of these changes is specifically the Doppler effect.
  12. Describe how Doppler ultrasound can provide information about blood flow.
  13. Explain how Doppler radar can determine whether an object is moving toward or away from a detector.
  14. Distinguish between redshift and blueshift and explain what each can indicate about an astronomical object's radial motion.
  15. A student says, "The pitch of an ambulance falls after it passes me because the driver changes the siren frequency." Evaluate this statement and use relative motion, emitted frequency, observed frequency, wavelength, and the Doppler effect to explain what actually happens.
 
 
 

2. Moving Sources and Observers

Learning outcomes
  • I can distinguish between moving sources and moving observers.
  • I can describe how each affects observed frequency.
  • I can interpret simple Doppler diagrams.
  • I can explain the compression and stretching of wavefronts.
  • I can compare different Doppler situations.

Moving Sources and Observers

The Doppler effect occurs when there is relative motion between a wave source and an observer. However, a moving source and a moving observer do not affect the wave in exactly the same way.

The key distinction is:

  • A moving source changes the spacing of the wavefronts in the medium.
  • A moving observer changes the rate at which the observer encounters existing wavefronts.

Both situations can change the observed frequency, but the physical reason for the change is different.

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7

Source and Observer

The source is the object producing the waves.

Examples include:

  • a loudspeaker
  • an ambulance siren
  • a train whistle
  • a vibrating tuning fork
  • a star producing light

The observer is the person or detector receiving the waves.

Examples include:

  • a person
  • a microphone
  • an ultrasound detector
  • a radar receiver
  • a telescope

Either the source, the observer, or both may be moving.


Relative Motion

The most important first question is:

Is the source-observer distance decreasing or increasing?

If they are approaching each other:

observed frequency increases

If they are moving apart:

observed frequency decreases

This rule works whether the source moves, the observer moves, or both move.

However, the wave pattern itself is different in each situation.


Four Basic Doppler Situations

The simplest situations are:

Situation Observed Frequency
Source moves toward observer Increases
Source moves away from observer Decreases
Observer moves toward source Increases
Observer moves away from source Decreases

A useful shortcut is:

toward → higher frequency

away → lower frequency


A Stationary Source and Stationary Observer

Begin with the simplest situation.

Suppose a sound source and observer are both stationary relative to the air.

The source produces:

fₛ = 500 Hz

The observer receives:

fₒ = 500 Hz

The wavefronts are evenly spaced around the stationary source.

There is no Doppler shift.


Moving Source

Now suppose the observer remains stationary while the source moves.

A moving source changes where each successive wavefront is produced.

This changes the spacing of the wavefronts.

Ahead of the source:

wavefronts are compressed

Behind the source:

wavefronts are stretched apart

This is the characteristic wave pattern of a moving source.

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7

Why a Moving Source Compresses Wavefronts

Imagine a siren moving toward an observer.

The siren emits one wave crest.

Before it emits the next crest, the siren moves forward.

The second crest therefore begins closer to the first crest in the forward direction.

The next crest begins even farther forward.

The result is:

smaller spacing between wavefronts

Therefore:

shorter wavelength


Moving Source Toward an Observer

For a source moving toward a stationary observer:

wavefronts compress

→ wavelength decreases

→ wavefronts arrive more frequently

→ observed frequency increases

For sound:

higher frequency → higher perceived pitch

Therefore:

approaching moving source → higher observed pitch


Moving Source Away from an Observer

Behind a moving source, each new wavefront begins farther from the previous one.

Therefore:

wavefronts spread apart

→ wavelength increases

→ wavefronts arrive less frequently

→ observed frequency decreases

For sound:

lower frequency → lower perceived pitch


The Wave Speed Does Not Change

Suppose an ambulance moves toward you.

It may seem reasonable to think:

"Since the ambulance is moving forward, the sound must travel faster."

That is not what happens.

In still air, the speed of sound is determined mainly by the properties of the air.

The ambulance changes the:

wavelength

not the normal propagation speed of sound through the air.


Moving Source and Wavelength

The wave equation is:

v = fλ

The source continues producing waves at its emitted frequency.

But because the source changes position between successive emissions, the wavelengths in front of and behind it are different.

Ahead:

shorter λ

Behind:

longer λ

This altered wavefront spacing is one of the easiest ways to recognize a moving source in a Doppler diagram.


Example: Moving Ambulance

Suppose an ambulance travels to the right.

An observer stands ahead of it.

The wavefronts between the ambulance and observer are compressed.

Therefore, the observer detects:

higher frequency

Another observer stands behind the ambulance.

The wavefronts reaching this observer are stretched apart.

Therefore, this observer detects:

lower frequency

The same source can therefore produce different observed frequencies at different locations.


Moving Observer

Now consider a different situation.

The source remains stationary, but the observer moves.

The stationary source produces evenly spaced wavefronts.

Therefore, unlike the moving-source situation:

the wavelength in the medium is not changed by the observer's motion.

Instead, the observer changes how rapidly they encounter the wavefronts.

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6

Observer Moving Toward the Source

Suppose an observer moves toward a stationary sound source.

The observer moves into the approaching wavefronts.

As a result, the observer encounters more wavefronts each second.

Therefore:

observed frequency increases

The wavelength in the air has not changed.

The observer simply encounters the wavefronts at a greater rate.


Observer Moving Away from the Source

Suppose the observer moves away from a stationary source.

The observer moves in the same general direction as the wavefronts.

The wavefronts take longer to catch the observer.

Therefore, fewer wavefronts reach the observer each second.

The result is:

observed frequency decreases

Again, the wavelength already present in the medium remains unchanged.


The Critical Difference

This distinction is extremely important.

Moving source:

changes wavefront spacing.

Moving observer:

does not change the wavefront spacing in the medium; instead, it changes how quickly the observer encounters the wavefronts.

Both can change observed frequency.


Comparing Moving Sources and Moving Observers

Moving Source Moving Observer
Source changes position between emissions Source remains in same position
Wavefront spacing changes Wavefront spacing in medium remains unchanged
Wavelength changes ahead/behind source Wavelength in medium stays the same
Observer may be stationary Source may be stationary
Approach gives higher fₒ Approach gives higher fₒ
Recession gives lower fₒ Recession gives lower fₒ

The final frequency trend is similar, but the physical mechanism is different.


Interpreting a Moving-Source Diagram

A moving-source diagram usually shows wavefronts that are:

  • crowded together on one side
  • spread apart on the opposite side

The source is moving toward the:

compressed wavefronts

and away from the:

stretched wavefronts

Therefore:

compressed side → higher observed frequency

stretched side → lower observed frequency


Finding the Direction of Source Motion

Suppose a diagram does not show a velocity arrow.

You can still determine the direction of motion.

Look for the side where the wavefronts are:

closest together

The source is moving toward that side.

For example:

wavefronts compressed on right → source moving right

wavefronts compressed on left → source moving left


Interpreting a Moving-Observer Diagram

For a stationary source, the wavefronts should remain evenly spaced.

Look at the observer's motion arrow.

If the observer moves toward the source:

frequency increases

If the observer moves away:

frequency decreases

Do not redraw the wavefronts as compressed simply because the observer is moving.

The observer's motion does not alter the waves already travelling through the medium.


Compression and Stretching of Wavefronts

The terms compression and stretching in a Doppler diagram describe the spacing between successive wavefronts.

Compressed wavefronts mean:

shorter wavelength

Stretched wavefronts mean:

longer wavelength

For a moving source:

front → compressed

behind → stretched

provided the source is moving slower than the wave speed.


Wavefront Spacing and Frequency

For a stationary observer in a stationary medium:

v = fλ

If the wave speed remains constant:

shorter λ → higher observed f

longer λ → lower observed f

Therefore:

compressed wavefronts → higher frequency

stretched wavefronts → lower frequency


Worked Example: Reading a Diagram

A sound source moves to the right.

The wavelength in front is:

λ = 0.60 m

The speed of sound is:

v = 340 m/s

The frequency detected by an observer ahead is:

f = v/λ

f = 340/0.60

f ≈ 567 Hz

Behind the source, suppose:

λ = 0.80 m

Then:

f = 340/0.80

f = 425 Hz

The observer ahead detects a much higher frequency than the observer behind.


Doppler Equation for a Moving Source

For a stationary observer and a source moving directly toward or away:

fₒ = fₛv/(v ∓ vₛ)

where:

fₒ = observed frequency

fₛ = emitted frequency

v = wave speed

vₛ = source speed

For an approaching source:

fₒ = fₛv/(v − vₛ)

For a receding source:

fₒ = fₛv/(v + vₛ)


Why the Signs Work for a Moving Source

When the source approaches:

denominator = v − vₛ

The denominator becomes smaller.

Therefore:

fₒ becomes larger

When the source recedes:

denominator = v + vₛ

The denominator becomes larger.

Therefore:

fₒ becomes smaller

This matches our physical prediction.


Worked Example: Moving Source Toward Observer

A siren emits:

fₛ = 600 Hz

The source moves toward a stationary observer at:

vₛ = 25 m/s

Assume:

v = 340 m/s

Use:

fₒ = fₛv/(v − vₛ)

fₒ = 600 × 340/(340 − 25)

fₒ = 204000/315

fₒ ≈ 648 Hz

The observed frequency is higher than 600 Hz.


Worked Example: Moving Source Away

The same source moves away at:

25 m/s.

Use:

fₒ = fₛv/(v + vₛ)

fₒ = 600 × 340/(340 + 25)

fₒ = 204000/365

fₒ ≈ 559 Hz

Therefore:

approaching → approximately 648 Hz

emitted → 600 Hz

receding → approximately 559 Hz


Doppler Equation for a Moving Observer

For a moving observer and stationary source:

fₒ = fₛ(v ± vₒ)/v

where:

vₒ = observer speed

For an observer moving toward the source:

fₒ = fₛ(v + vₒ)/v

For an observer moving away:

fₒ = fₛ(v − vₒ)/v


Worked Example: Observer Moving Toward Source

A stationary source produces:

fₛ = 600 Hz

An observer approaches at:

vₒ = 25 m/s

Use:

fₒ = 600(340 + 25)/340

fₒ = 600 × 365/340

fₒ ≈ 644 Hz

The observed frequency increases.


Worked Example: Observer Moving Away

The observer now moves away at:

25 m/s.

fₒ = 600(340 − 25)/340

fₒ = 600 × 315/340

fₒ ≈ 556 Hz

The observed frequency decreases.


Same Speed Does Not Give Exactly the Same Shift

Compare the previous examples.

Source approaching at 25 m/s:

fₒ ≈ 648 Hz

Observer approaching at 25 m/s:

fₒ ≈ 644 Hz

These are similar but not exactly equal.

Why?

Because moving sources and moving observers affect sound differently.

A moving source changes:

wavelength

A moving observer changes:

wavefront encounter rate

This is why the equations are different.


Both Source and Observer Moving

Sometimes both objects move.

For sound in a stationary medium, a commonly used equation is:

fₒ = fₛ(v ± vₒ)/(v ∓ vₛ)

The signs must be chosen according to whether the motions bring the source and observer closer together or farther apart.

A useful physical check is always:

approaching → fₒ should increase

receding → fₒ should decrease

If your calculation gives the opposite result, check the signs.


Worked Example: Both Approaching

A source emits:

fₛ = 500 Hz

The source moves toward the observer at:

vₛ = 20 m/s

The observer moves toward the source at:

vₒ = 10 m/s

Assume:

v = 340 m/s

Use:

fₒ = fₛ(v + vₒ)/(v − vₛ)

fₒ = 500(340 + 10)/(340 − 20)

fₒ = 500 × 350/320

fₒ ≈ 547 Hz

Since they are approaching:

fₒ > fₛ

as expected.


Both Moving in the Same Direction

Suppose a source and observer are both moving to the right.

You cannot determine the Doppler shift simply by seeing that they move in the same direction.

You must compare their speeds.

For example:

source behind moving faster than observer → separation decreases

Therefore:

approaching

source behind moving slower than observer → separation increases

Therefore:

receding

Always determine whether their distance is changing.


Example: Catching Up

A car producing a horn travels at:

30 m/s.

An observer in another vehicle ahead travels in the same direction at:

20 m/s.

The source is gaining on the observer.

Their separation is decreasing.

Therefore, they are approaching relative to one another.

The observer detects a frequency:

higher than the emitted frequency

for the usual sound Doppler situation.


Example: Pulling Away

Now suppose the observer ahead travels at:

35 m/s

while the source behind travels at:

25 m/s.

The distance between them increases.

Therefore:

they are receding

The observed frequency is:

lower than the emitted frequency


Sideways Motion

Suppose a source moves across an observer's field of view rather than directly toward or away.

The Doppler shift depends on the component of velocity along the line connecting source and observer.

This is the:

radial component of velocity

Motion directly toward or away gives the largest ordinary Doppler effect for a given speed.

Motion perpendicular to the line of sight has no instantaneous classical radial Doppler shift at the point of closest approach.


A Vehicle Passing an Observer

Consider a car approaching a person standing beside a road.

Before the car passes:

the car has a velocity component toward the observer.

Therefore:

fₒ > fₛ

After the car passes:

the car has a velocity component away from the observer.

Therefore:

fₒ < fₛ

Near the moment of closest approach, the radial component changes sign.

This produces the familiar change from higher to lower pitch.

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8

Comparing Doppler Situations

Source Observer Separation Observed Frequency
Stationary Stationary Constant fₒ = fₛ
Toward observer Stationary Decreasing fₒ > fₛ
Away from observer Stationary Increasing fₒ < fₛ
Stationary Toward source Decreasing fₒ > fₛ
Stationary Away from source Increasing fₒ < fₛ
Both approaching Moving Decreasing fₒ > fₛ
Both separating Moving Increasing fₒ < fₛ

Moving Source vs Moving Observer Diagrams

A useful way to distinguish the diagrams is to inspect the wavefronts.

Moving source

Wavefront spacing is uneven.

There are compressed wavefronts ahead and stretched wavefronts behind.

Moving observer

If the source is stationary, wavefront spacing remains symmetrical and even.

The observer simply moves through those wavefronts.

This visual distinction is extremely useful in examination questions.


Interpreting Arrows

Doppler diagrams may contain several types of arrows.

A source arrow shows:

source velocity

An observer arrow shows:

observer velocity

Wave propagation arrows show:

direction of wave travel

Do not confuse the motion of the source or observer with the motion of the waves.


Source Motion and Wave Motion Are Different

Suppose a source moves right while producing sound.

The sound itself spreads outward in many directions through the medium.

Some waves travel:

  • ahead of the source
  • behind the source
  • sideways from the source

The source motion changes where successive wavefronts originate.

It does not mean every sound wave simply moves in the same direction as the source.


Everyday Example: Train and Passenger

Imagine a stationary train whistle beside a platform while a passenger moves toward it on another train.

The whistle produces evenly spaced wavefronts.

The moving passenger encounters these wavefronts more frequently.

This is a:

moving-observer Doppler effect

Now imagine the passenger standing still while the whistle itself approaches on a moving train.

The wavefronts are compressed ahead of the train.

This is a:

moving-source Doppler effect

Both produce higher observed frequency, but for different reasons.


Doppler Ultrasound

Moving-source and moving-observer ideas are also useful when thinking about medical Doppler ultrasound.

Ultrasound is transmitted toward moving blood cells.

The blood cells interact with and reflect the waves.

Their motion causes frequency shifts in the returning ultrasound.

The equipment analyzes these shifts to determine information about:

  • direction of blood flow
  • relative speed of blood flow
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9

Radar

Doppler radar sends electromagnetic waves toward moving targets.

The waves reflect from the target.

The frequency of the returning wave differs from the transmitted frequency when the target has motion toward or away from the radar.

This allows radar to measure:

radial velocity

Applications include:

  • vehicle speed detection
  • aircraft tracking
  • weather radar
  • navigation

Astronomy

In astronomy, the observer is often approximately stationary relative to the measurement system while a star or galaxy has motion toward or away from us.

Motion away produces a shift toward longer wavelengths.

Motion toward produces a shift toward shorter wavelengths.

Astronomers use these shifts to investigate the radial motion of astronomical objects.


What Happens as Source Speed Increases?

As a sound source moves faster toward an observer:

  • wavefront compression increases
  • forward wavelength decreases
  • observed frequency increases

As its speed approaches the speed of sound, the wavefronts ahead become increasingly compressed.

This leads to a more extreme wave phenomenon.


Approaching the Speed of Sound

When an object moves through air at approximately the speed of sound, successive pressure disturbances can build up into a strong wavefront.

Instead of ordinary separated wavefronts moving ahead of the source, disturbances accumulate.

This is associated with the formation of a:

shock wave


Supersonic Motion

If an object travels faster than sound:

v_source > v_sound

it outruns the sound disturbances it produces.

The wavefronts form a cone-shaped pattern called a:

Mach cone

When the shock wave passes an observer, it can be heard as a:

sonic boom

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The Sonic Boom Is Not Just an Extreme Pitch Shift

A sonic boom is associated with a shock wave produced by supersonic motion.

It should not simply be described as an extremely high-pitched Doppler sound.

The physics involves the accumulation and geometry of pressure disturbances into a shock front.

It is related to moving-source wave behaviour but represents a different regime from the ordinary Doppler effect.


A Complete Moving-Source Example

A source moves toward a stationary observer.

The source emits sound at:

600 Hz.

Because the source moves forward between successive emissions:

  • wavefronts ahead become compressed
  • forward wavelength decreases
  • sound speed through the stationary air remains approximately unchanged
  • observed frequency increases

The observer therefore detects:

fₒ > 600 Hz

After the source passes:

  • wavefronts reaching the observer are more widely spaced
  • wavelength is greater
  • observed frequency is lower

Therefore:

fₒ < 600 Hz


A Complete Moving-Observer Example

A stationary source emits:

600 Hz.

The wavefronts in the air are evenly spaced.

An observer moves toward the source.

The observer encounters more than 600 wavefront cycles per second.

Therefore:

fₒ > 600 Hz

The observer then turns around and moves away.

They encounter fewer wavefronts each second.

Therefore:

fₒ < 600 Hz

Throughout this process, the source remains stationary and the wavelength in the air remains unchanged.


A Reliable Strategy for Doppler Diagrams

When given a Doppler diagram:

  1. Locate the source.
  2. Locate the observer.
  3. Identify which one is moving.
  4. Examine the wavefront spacing.
  5. Uneven wavefront spacing suggests a moving source.
  6. Compressed wavefronts show the direction toward which the source moves.
  7. Even wavefront spacing with a moving observer suggests a stationary source.
  8. Determine whether source and observer are approaching or separating.
  9. Approaching means higher observed frequency.
  10. Separating means lower observed frequency.
  11. Distinguish wavelength changes from observer encounter-rate changes.
  12. Check whether your explanation matches the diagram.

A Reliable Strategy for Calculations

For numerical Doppler questions:

  1. Write the emitted frequency fₛ.
  2. Write the wave speed v.
  3. Identify source speed vₛ if present.
  4. Identify observer speed vₒ if present.
  5. Determine whether each motion is toward or away.
  6. Predict whether fₒ should be higher or lower than fₛ.
  7. Choose the correct Doppler equation.
  8. Substitute values carefully.
  9. Calculate fₒ.
  10. Compare the result with your prediction.
  11. If approaching but fₒ < fₛ, recheck the signs.
  12. Include Hz in the final answer.

Common Mistakes

Thinking a moving source and moving observer affect waves identically

They can produce similar frequency shifts, but the physical mechanisms differ.

Thinking a moving observer compresses the wavefronts

The observer does not change the wavelength already present in the medium.

Thinking a moving source changes the speed of sound

It changes wavefront spacing, not the ordinary sound speed through stationary air.

Looking only at direction arrows

Always determine whether the separation between source and observer increases or decreases.

Assuming two objects moving in the same direction are receding

A faster object behind may be catching the object ahead.

Thinking compressed wavefronts mean lower frequency

For the same wave speed, compressed wavefronts mean shorter wavelength and higher frequency.

Thinking stretched wavefronts mean higher frequency

Greater wavelength corresponds to lower frequency when wave speed is unchanged.

Using the moving-source equation for a moving observer

The equations are different because the physical situations are different.

Assuming equal source and observer speeds produce exactly equal Doppler shifts

For sound in a medium, equal source and observer speeds generally do not produce exactly identical shifts.

Ignoring radial motion

The ordinary Doppler shift depends on motion toward or away along the source-observer line.

Thinking a sonic boom is simply a high-pitched Doppler effect

A sonic boom is produced by a shock wave associated with supersonic motion.


Key Terms

Source — object or system producing waves.

Observer — person or detector receiving waves.

Relative motion — motion of the source and observer compared with one another.

Doppler effect — observed frequency change caused by relative motion.

Emitted frequency (fₛ) — frequency produced by the source.

Observed frequency (fₒ) — frequency detected by the observer.

Moving source — wave source whose position changes relative to the medium and observer.

Moving observer — detector whose position changes relative to the source and wavefronts.

Wavefront — line or surface connecting points of a wave in the same phase.

Wavefront compression — reduced spacing between successive wavefronts.

Wavefront stretching — increased spacing between successive wavefronts.

Wavelength (λ) — distance between corresponding points on consecutive waves.

Radial velocity — velocity component toward or away from an observer.

Approaching — motion that decreases source-observer separation.

Receding — motion that increases source-observer separation.

Shock wave — strong disturbance formed when wave disturbances accumulate due to sufficiently rapid source motion.

Mach cone — cone-shaped shock-wave pattern associated with supersonic motion.

Sonic boom — sound produced when a shock wave from a supersonic object passes an observer.


Key Takeaways

  • Both moving sources and moving observers can produce the Doppler effect.
  • Approaching motion increases observed frequency.
  • Receding motion decreases observed frequency.
  • A moving source changes the spacing of wavefronts in the medium.
  • Wavefronts are compressed ahead of an approaching moving source.
  • Wavefronts are stretched behind a moving source.
  • Compressed wavefronts have shorter wavelength.
  • Stretched wavefronts have longer wavelength.
  • A moving observer does not change the wavelength already present in the medium.
  • A moving observer changes how rapidly they encounter wavefronts.
  • An observer moving toward a source encounters wavefronts more frequently.
  • An observer moving away encounters them less frequently.
  • Moving-source and moving-observer Doppler shifts are similar but not physically identical.
  • Their Doppler equations are therefore different for waves such as sound travelling through a medium.
  • The source's motion does not simply increase or decrease the normal speed of sound.
  • A Doppler diagram with uneven wavefront spacing usually represents a moving source.
  • Compressed wavefronts indicate the direction of source motion.
  • For two objects moving in the same direction, their relative speeds determine whether they approach or separate.
  • The Doppler effect depends primarily on the radial component of relative motion.
  • Doppler ultrasound, radar, astronomy, and speed measurement all use frequency shifts caused by motion.
  • At sufficiently high source speeds, ordinary moving-source behaviour leads toward shock-wave phenomena.
  • Supersonic objects can produce Mach cones and sonic booms.

Check Your Understanding

  1. Distinguish between a moving source and a moving observer.
  2. Explain what happens to the wavefronts in front of a sound source moving through still air.
  3. Explain what happens to the wavefronts behind the moving source.
  4. Why does an observer ahead of an approaching source detect a higher frequency?
  5. A stationary source produces evenly spaced wavefronts. An observer moves toward the source. Explain why the observed frequency increases even though the wavelength in the medium remains unchanged.
  6. Compare how a moving source and a moving observer produce a Doppler shift.
  7. A diagram shows a source with wavefronts tightly packed on its right side and widely spaced on its left side. Determine the direction in which the source is moving and explain your reasoning.
  8. A 600 Hz siren moves toward a stationary observer at 25 m/s. If the speed of sound is 340 m/s, calculate the observed frequency.
  9. Calculate the observed frequency if the same 600 Hz source moves away at 25 m/s.
  10. A stationary 600 Hz source is approached by an observer travelling at 25 m/s. Calculate the observed frequency and compare it with the moving-source result from Question 8.
  11. Two vehicles travel in the same direction. A siren source behind travels at 30 m/s while the observer ahead travels at 20 m/s. Are they approaching or receding? Predict whether the observed frequency is higher or lower than the emitted frequency.
  12. Explain why the speed of sound through the air does not increase simply because the sound source moves forward.
  13. Explain why motion directly toward or away from an observer produces a stronger ordinary Doppler effect than motion perpendicular to the source-observer line.
  14. Describe how you could distinguish a moving-source diagram from a moving-observer diagram by examining the wavefronts.
  15. A student says, "Moving a source toward an observer and moving an observer toward a source are exactly the same because both produce a higher frequency." Evaluate this statement. Explain what is similar about the two situations, what is physically different, and how the wavefront pattern changes in each case.
 
 
 

3. Doppler Effect for Sound

Learning outcomes
  • I can explain why the pitch of a siren changes.
  • I can describe the Doppler effect using sound waves.
  • I can predict changes in pitch.
  • I can solve simple Doppler problems conceptually.
  • I can identify everyday examples.

Doppler Effect for Sound

The Doppler effect is the apparent change in the frequency of a sound caused by relative motion between the sound source and the observer.

A familiar example is an emergency vehicle passing you with its siren sounding. As it approaches, the siren seems to have a higher pitch. After it passes and moves away, the pitch becomes lower.

The siren does not need to change the frequency it produces. The change you hear occurs because the motion of the source changes how frequently the sound wavefronts reach you.

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8

Sound Waves and Frequency

Sound is a mechanical longitudinal wave.

In air, sound travels as alternating regions of:

  • compression
  • rarefaction

The frequency of a sound is the number of complete wave cycles passing a point each second.

Frequency is measured in:

hertz (Hz)

For example:

500 Hz = 500 cycles per second

Frequency is strongly related to the pitch we hear.

higher frequency → higher pitch

lower frequency → lower pitch


Pitch and Frequency

Pitch is the perception of how high or low a sound seems.

A high-frequency sound is generally perceived as having a high pitch.

Examples include:

  • whistle
  • small bell
  • high piano note

A low-frequency sound is generally perceived as having a low pitch.

Examples include:

  • bass guitar
  • large drum
  • low piano note

The Doppler effect changes the observed frequency, which causes the observed pitch to change.


The Siren Example

Imagine standing beside a road.

An ambulance approaches with its siren producing a constant frequency.

As it approaches:

you hear a higher pitch

As it passes:

the pitch drops

As it moves away:

you hear a lower pitch

This characteristic change is caused by the:

Doppler effect

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Why the Siren's Pitch Changes

The siren produces sound waves continuously while the ambulance moves.

Between producing one wavefront and the next, the ambulance changes position.

In front of the ambulance:

wavefronts become closer together

Behind the ambulance:

wavefronts become farther apart

Therefore, observers in front and behind receive different wave patterns.


In Front of the Moving Siren

The ambulance moves toward the wavefronts it has already produced.

Each new wavefront begins slightly closer to the previous one.

Therefore:

wavefront spacing decreases

This means:

wavelength decreases

Since sound speed through the same air remains approximately constant:

shorter wavelength → higher observed frequency

Therefore:

approaching siren → higher pitch


Behind the Moving Siren

Behind the ambulance, each successive wavefront begins farther forward than the previous one.

The wavefronts behind become:

farther apart

Therefore:

wavelength increases

With approximately constant sound speed:

longer wavelength → lower observed frequency

Therefore:

receding siren → lower pitch


The Essential Doppler Rule

For sound, remember:

approaching → higher observed frequency → higher pitch

receding → lower observed frequency → lower pitch

This rule solves many conceptual Doppler questions without any calculation.


Emitted and Observed Frequency

It is important to distinguish between two frequencies.

Emitted frequency

The frequency actually produced by the source.

Symbol:

fₛ

Observed frequency

The frequency detected by the observer.

Symbol:

fₒ

During a Doppler shift:

fₒ may be different from fₛ


Example of Emitted and Observed Frequency

Suppose a siren continuously emits:

700 Hz

When the ambulance approaches, an observer might detect a frequency greater than:

700 Hz

After the ambulance passes and moves away, the observer might detect a frequency below:

700 Hz

The siren itself can continue emitting:

700 Hz

The observed frequency changes because of relative motion.


Wavefront Compression

A wavefront represents points on a wave that are at the same stage of oscillation.

For a moving sound source, the wavefronts in front become compressed.

Compressed wavefronts mean:

shorter wavelength

Using:

v = fλ

if v remains approximately constant:

smaller λ → larger f

Therefore, an observer in front detects a higher frequency.

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8

Wavefront Stretching

Behind the source, wavefronts are stretched farther apart.

Stretched wavefronts mean:

longer wavelength

If sound speed remains approximately constant:

larger λ → smaller f

Therefore, an observer behind the moving source detects a lower frequency.


Comparing the Wavefronts

Position Wavefront Spacing Wavelength Observed Frequency Pitch
In front of approaching source Compressed Shorter Higher Higher
Behind receding source Stretched Longer Lower Lower

This table summarizes the most important relationship for a moving sound source.


The Speed of Sound Does Not Increase

A common mistake is to think that sound travels faster because the ambulance is moving toward the observer.

This is not what causes the Doppler effect.

The speed of sound through still air is determined mainly by the properties of the air, especially temperature.

The moving source changes:

wavefront spacing

rather than simply adding its speed to the speed of sound.


The Wave Equation

Sound waves obey:

v = fλ

where:

v = wave speed

f = frequency

λ = wavelength

For sound travelling through the same air, v remains approximately constant.

Therefore:

shorter wavelength → higher frequency

longer wavelength → lower frequency

This helps explain the Doppler effect for a moving source.


Conceptual Example: Approaching Car

A car horn approaches a stationary observer.

Question:

Does the observer hear a higher or lower pitch?

Reasoning:

  1. The car approaches.
  2. Wavefronts ahead are compressed.
  3. Wavelength is shorter.
  4. Wavefronts reach the observer more frequently.
  5. Observed frequency increases.

Answer:

higher pitch

No numerical calculation is required.


Conceptual Example: Receding Train

A train moves away while sounding its whistle.

Question:

How does the observed pitch compare with the emitted pitch?

Reasoning:

  1. Train is moving away.
  2. Wavefronts reaching the observer are farther apart.
  3. Observed wavelength is longer.
  4. Fewer wave cycles reach the observer each second.
  5. Observed frequency is lower.

Answer:

lower pitch


What Happens When the Vehicle Passes?

Before a vehicle passes:

source approaching → higher observed frequency

After it passes:

source receding → lower observed frequency

Therefore, the listener hears a noticeable drop in pitch.

The change can sound sudden because the component of the vehicle's velocity toward the observer changes to a component away from the observer as it passes.


Source Moving Toward an Observer

For a moving sound source:

source approaches

→ wavefront compression

→ shorter wavelength

→ higher observed frequency

→ higher pitch

This is one of the most important cause-and-effect chains to remember.


Source Moving Away from an Observer

Similarly:

source recedes

→ wavefront stretching

→ longer wavelength

→ lower observed frequency

→ lower pitch


A Moving Observer

The observer can also move.

Suppose the sound source is stationary.

Its wavefronts remain evenly spaced in the air.

If the observer moves toward the source, the observer encounters wavefronts more frequently.

Therefore:

observer moving toward source → higher observed frequency

If the observer moves away:

observer moving away from source → lower observed frequency


Moving Source vs Moving Observer

There is an important difference.

Moving source

Changes the spacing of wavefronts in the medium.

Moving observer

Does not change the spacing of the existing wavefronts. Instead, the observer changes how rapidly they encounter them.

Both situations can produce a Doppler shift.


Both Moving

The source and observer can both move.

The simplest way to make a conceptual prediction is to ask:

Is the distance between them decreasing or increasing?

If decreasing:

higher observed frequency

If increasing:

lower observed frequency

This is often more useful than focusing only on the individual directions of motion.


Same Direction Does Not Necessarily Mean Moving Apart

Suppose a siren and observer both travel to the right.

The siren is behind.

If the siren travels faster than the observer, it catches up.

Their separation decreases.

Therefore:

observed frequency increases

If the observer travels faster and pulls away:

separation increases

Therefore:

observed frequency decreases

Always consider the change in distance between source and observer.


Everyday Doppler Examples

The Doppler effect can be heard from many moving sound sources:

  • ambulance sirens
  • police sirens
  • fire engines
  • train whistles
  • car horns
  • motorcycles
  • racing cars
  • aircraft
  • fast-moving machinery

The effect is most noticeable when the source moves quickly compared with the speed of sound.


Train Whistle

Imagine standing at a railway station.

A train approaches while sounding its whistle.

Before the train passes:

pitch is higher

As the train passes:

pitch drops

After the train passes:

pitch is lower

The whistle does not need to change its emitted frequency.

The changing pitch results from the Doppler effect.


Racing Cars

The Doppler effect is particularly noticeable with racing vehicles.

As a race car approaches:

engine frequencies are shifted upward

After it passes:

frequencies are shifted downward

The familiar change in engine sound is partly a Doppler effect.

The engine's actual operating frequency may also change as the driver accelerates or changes gears, so real vehicle sounds can be more complicated than the idealized model.


Aircraft

Aircraft can also produce noticeable Doppler shifts.

As an aircraft approaches:

observed sound frequencies increase

As it recedes:

observed frequencies decrease

The effect can be combined with delays caused by the finite speed of sound, particularly for fast aircraft.


Doppler Equation for a Moving Source

For a stationary observer and a sound source moving directly toward or away from the observer:

fₒ = fₛv/(v ∓ vₛ)

where:

fₒ = observed frequency

fₛ = emitted frequency

v = speed of sound

vₛ = speed of source

For an approaching source:

fₒ = fₛv/(v − vₛ)

For a receding source:

fₒ = fₛv/(v + vₛ)


Worked Example: Approaching Siren

An ambulance emits:

fₛ = 800 Hz

It approaches a stationary observer at:

vₛ = 20 m/s

Take the speed of sound as:

v = 340 m/s

Use:

fₒ = fₛv/(v − vₛ)

fₒ = 800 × 340/(340 − 20)

fₒ = 272000/320

fₒ = 850 Hz

The observer hears:

850 Hz

This is higher than the emitted frequency.


Worked Example: Receding Siren

The same ambulance moves away at:

20 m/s.

Use:

fₒ = fₛv/(v + vₛ)

fₒ = 800 × 340/(340 + 20)

fₒ = 272000/360

fₒ ≈ 756 Hz

Therefore:

approaching → 850 Hz

emitted → 800 Hz

receding → 756 Hz

This matches our conceptual prediction.


Predict Before Calculating

Before using an equation, always make a prediction.

Ask:

Is the source approaching or receding?

If approaching:

your calculated answer must satisfy:

fₒ > fₛ

If receding:

your answer must satisfy:

fₒ < fₛ

This is an excellent way to catch calculation or sign errors.


Conceptual Doppler Problems

Many Doppler problems do not require an equation.

For example:

A motorcycle approaches a pedestrian.

Prediction:

higher observed frequency.

A train moves away from a station.

Prediction:

lower observed frequency.

A cyclist moves toward a stationary bell.

Prediction:

higher observed frequency.

A car and observer remain the same distance apart.

Prediction:

no ordinary Doppler shift due to radial relative motion.


Which Observer Hears the Highest Frequency?

Suppose a moving siren has three observers.

Observer A is directly ahead.

Observer B is directly behind.

Observer C is mostly to the side.

Observer A experiences the strongest approaching radial motion and therefore hears a higher frequency.

Observer B experiences receding motion and hears a lower frequency.

Observer C experiences a smaller radial component of the source's velocity and therefore usually experiences a smaller Doppler shift at that instant.


Radial Motion

The ordinary Doppler effect depends primarily on motion along the line connecting the source and observer.

This is called:

radial motion

Motion directly toward the observer produces a strong positive frequency shift.

Motion directly away produces a strong negative frequency shift.

Purely sideways motion has no instantaneous classical radial Doppler shift at the moment when the motion is exactly perpendicular to the source-observer line.


Doppler Effect and Loudness

An approaching siren usually becomes:

  • louder
  • higher in pitch

A receding siren usually becomes:

  • quieter
  • lower in pitch

However, these are caused by different effects.

Pitch change

is caused by the Doppler frequency shift.

Loudness change

is mainly caused by changing distance and sound intensity.

Therefore:

louder does not mean higher frequency.


Doppler Effect and Amplitude

The Doppler effect concerns:

frequency

It does not fundamentally require a change in amplitude.

A sound could theoretically undergo a Doppler frequency shift while maintaining similar amplitude.

In everyday situations, amplitude often changes because the distance between source and observer changes.


Doppler Ultrasound

The Doppler effect for sound has important medical applications.

Doppler ultrasound sends high-frequency sound waves into the body.

The waves can reflect from moving blood cells.

Because the reflecting cells are moving, the frequency of the returning ultrasound changes.

Doctors can analyze this frequency shift to obtain information about blood flow.

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9

Measuring Blood Flow

Doppler ultrasound can provide information about:

  • direction of blood flow
  • relative blood-flow speed
  • circulation
  • heart function
  • blood vessels

Blood moving toward the ultrasound transducer produces a different frequency shift from blood moving away.

The Doppler effect therefore allows motion inside the body to be studied without surgery.


Ultrasound Uses Reflected Sound

Doppler ultrasound combines more than one wave behaviour.

The ultrasound first:

travels into the body

It then:

reflects from moving structures

The motion produces:

a Doppler frequency shift

The returning sound is detected and analyzed.

This is an excellent example of several wave concepts working together in one technology.


Bats and Echolocation

Bats produce high-frequency sounds and detect returning echoes.

This process is called:

echolocation

Reflection provides information about distance.

Doppler shifts can also provide information about relative motion in species that make use of such frequency changes.

This can help an animal obtain information about moving prey or surroundings.


Speed Measurement

The Doppler principle can be used to determine motion by measuring frequency changes.

For sound-based systems, a known frequency is transmitted.

If the sound reflects from a moving object, the returned frequency may be shifted.

The size and direction of the shift can provide information about motion.

Similar principles are used with electromagnetic waves in radar.


Sound from Rotating Objects

The Doppler effect can also occur when parts of a rotating object move alternately toward and away from an observer.

For example, rotating machinery can produce complicated frequency patterns.

Engineers can analyze sound and vibration frequencies to investigate:

  • machine speed
  • vibration
  • faults
  • rotating components

Wave analysis is therefore useful in engineering diagnostics.


Siren Passing at Constant Speed

Consider a vehicle moving past an observer at constant speed.

Even though the vehicle's speed remains constant, the observed frequency changes.

Why?

Because the radial component of its velocity changes.

While approaching:

radial motion is toward the observer.

After passing:

radial motion is away.

Therefore, constant vehicle speed does not mean constant observed frequency.


Does the Pitch Change Exactly at the Passing Point?

In an idealized geometry, the source's radial velocity relative to an observer beside its path becomes zero at the instant of closest approach.

The observed frequency changes continuously with geometry.

In everyday listening, the transition can sound like a rapid drop because the source moves quickly from approaching to receding.

This is more accurate than imagining that the siren itself suddenly changes frequency.


Sound Speed and Temperature

The speed of sound in air depends on conditions, particularly temperature.

A commonly used classroom value is:

340 m/s

although the actual value varies.

For example, around room temperature it is often closer to:

343 m/s

Doppler calculations normally provide or specify the sound speed to use.


A Complete Siren Example

An ambulance emits a constant:

750 Hz

Before passing an observer, it approaches.

Therefore:

  • wavefronts ahead are compressed
  • wavelength decreases
  • observed frequency is greater than 750 Hz
  • observed pitch is higher

After passing:

  • wavefronts reaching the observer are stretched apart
  • wavelength increases
  • observed frequency is below 750 Hz
  • observed pitch is lower

The emitted frequency remains:

750 Hz

The observed change is caused by relative motion.


A Complete Conceptual Comparison

Consider four situations.

A. Source approaches stationary observer

Observed frequency:

increases

B. Source recedes from stationary observer

Observed frequency:

decreases

C. Observer approaches stationary source

Observed frequency:

increases

D. Observer recedes from stationary source

Observed frequency:

decreases

Therefore, the simplest conceptual rule remains:

distance decreasing → frequency increasing

distance increasing → frequency decreasing


Interpreting Doppler Diagrams

When a diagram shows circular sound wavefronts around a moving source, examine their spacing.

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7

If wavefronts are closer together:

shorter wavelength

→ higher observed frequency

→ higher pitch

If wavefronts are farther apart:

longer wavelength

→ lower observed frequency

→ lower pitch

The source is moving toward the compressed side.


A Reliable Strategy for Conceptual Doppler Problems

When solving a Doppler question:

  1. Identify the sound source.
  2. Identify the observer.
  3. Determine which one is moving.
  4. Decide whether the distance between them is decreasing or increasing.
  5. Decreasing distance means approaching.
  6. Increasing distance means receding.
  7. Approaching means higher observed frequency.
  8. Receding means lower observed frequency.
  9. For sound, convert frequency prediction into pitch.
  10. If a moving source is shown, inspect wavefront spacing.
  11. Compressed wavefronts mean shorter wavelength and higher frequency.
  12. Stretched wavefronts mean longer wavelength and lower frequency.
  13. Distinguish emitted frequency from observed frequency.
  14. Do not confuse frequency changes with loudness changes.
  15. Check that your explanation matches the physical situation.

A Reliable Strategy for Numerical Problems

If a calculation is required:

  1. Write the emitted frequency fₛ.
  2. Write the speed of sound v.
  3. Write the source speed vₛ if given.
  4. Determine whether the source approaches or recedes.
  5. Predict whether fₒ should be higher or lower than fₛ.
  6. Select the appropriate equation.
  7. Substitute the values.
  8. Calculate the observed frequency.
  9. Include Hz.
  10. Compare the result with your prediction.

For example:

approaching 700 Hz source

→ answer must be greater than 700 Hz

receding 700 Hz source

→ answer must be less than 700 Hz


Common Mistakes

Thinking the siren itself changes frequency as it passes

The emitted frequency can remain constant while the observed frequency changes.

Thinking an approaching source produces a lower pitch

Approaching means higher observed frequency and higher pitch.

Thinking a receding source produces a higher pitch

Receding means lower observed frequency and lower pitch.

Thinking compressed wavefronts mean lower frequency

Compressed wavefronts have shorter wavelength and correspond to higher observed frequency for the same sound speed.

Thinking the source makes sound travel faster

The source changes wavefront spacing rather than simply adding its velocity to the sound speed.

Confusing pitch with loudness

Pitch is strongly related to frequency. Loudness is related to intensity and perception.

Using loudness as evidence of the Doppler effect

The Doppler effect specifically concerns frequency.

Thinking only the source can move

Motion of the observer can also produce a Doppler shift.

Looking only at direction instead of relative motion

Two objects can move in the same direction while still approaching one another.

Forgetting to predict before calculating

A quick higher/lower prediction is one of the easiest ways to detect a wrong numerical answer.


Key Terms

Doppler effect — change in observed frequency caused by relative motion between a wave source and observer.

Sound wave — mechanical longitudinal wave produced by vibrations and transmitted through a medium.

Source — object producing the sound.

Observer — person or detector receiving the sound.

Emitted frequency (fₛ) — frequency actually produced by the sound source.

Observed frequency (fₒ) — frequency detected by the observer.

Pitch — perception associated strongly with sound frequency.

Frequency — number of wave cycles passing a point each second.

Hertz (Hz) — unit of frequency equal to one cycle per second.

Wavelength (λ) — distance between corresponding points on consecutive waves.

Wavefront — representation of points on a wave that are at the same phase.

Wavefront compression — reduction in spacing between successive wavefronts ahead of a moving source.

Wavefront stretching — increase in spacing between successive wavefronts behind a moving source.

Approaching — relative motion that decreases source-observer separation.

Receding — relative motion that increases source-observer separation.

Relative motion — motion of the source and observer compared with one another.

Radial motion — component of motion toward or away from an observer.

Doppler shift — difference between emitted and observed frequencies.

Doppler ultrasound — medical technique that uses frequency shifts in ultrasound to investigate moving structures such as blood.

Echolocation — use of reflected sound to obtain information about objects and surroundings.


Key Takeaways

  • The Doppler effect explains why a moving siren appears to change pitch.
  • Sound is a mechanical longitudinal wave.
  • Frequency is measured in hertz.
  • Higher frequency is generally perceived as higher pitch.
  • Lower frequency is generally perceived as lower pitch.
  • An approaching source produces a higher observed frequency.
  • A receding source produces a lower observed frequency.
  • The emitted frequency can remain constant while the observed frequency changes.
  • A moving source compresses wavefronts ahead of it.
  • Compressed wavefronts have shorter wavelength.
  • Shorter wavelength corresponds to higher observed frequency when sound speed is unchanged.
  • A moving source stretches wavefronts behind it.
  • Stretched wavefronts have longer wavelength.
  • Longer wavelength corresponds to lower observed frequency.
  • The moving source does not simply make sound travel faster.
  • A moving observer can also experience a Doppler shift.
  • An observer approaching a source detects a higher frequency.
  • An observer moving away detects a lower frequency.
  • Relative motion toward or away is more important than simply asking which object moves.
  • Changes in loudness and changes in pitch have different causes.
  • Sirens, train whistles, car horns, motorcycles, racing vehicles, and aircraft provide everyday examples.
  • Doppler ultrasound uses frequency shifts to study blood flow.
  • The size of the Doppler shift can provide information about relative motion.
  • Conceptual Doppler problems can often be solved simply by deciding whether the source and observer are approaching or receding.

Check Your Understanding

  1. Define the Doppler effect for sound.
  2. Explain why an approaching ambulance siren sounds higher in pitch than its emitted pitch.
  3. Explain why the same siren sounds lower in pitch after the ambulance passes and moves away.
  4. Distinguish between emitted frequency and observed frequency.
  5. A siren emits a constant frequency of 700 Hz. An observer hears 750 Hz. Is the source most likely approaching or receding? Explain.
  6. Another observer hears the same 700 Hz siren at 660 Hz. Is the source approaching or receding?
  7. Describe what happens to the wavelength of sound in front of a moving source.
  8. Describe what happens to the wavelength behind a moving source.
  9. Explain why the speed of sound does not simply increase because a sound source moves toward an observer.
  10. A stationary source produces a 500 Hz sound. An observer moves toward the source. Predict whether the observed frequency is greater than, equal to, or less than 500 Hz and explain why.
  11. An ambulance emits an 800 Hz siren and approaches a stationary observer at 20 m/s. Using a sound speed of 340 m/s, calculate the observed frequency.
  12. Calculate the observed frequency when the same ambulance moves away at 20 m/s.
  13. An approaching siren becomes both louder and higher in pitch. Explain why only the pitch change is specifically the Doppler effect.
  14. Describe how Doppler ultrasound uses changes in sound frequency to provide information about blood flow.
  15. A student says, "When an ambulance drives toward me, its siren sounds higher because the ambulance pushes the sound forward and makes the sound travel faster." Evaluate this statement. Explain the actual changes in wave speed, wavelength, observed frequency, and pitch.

4. Doppler Effect for Light

Learning outcomes
  • I can explain redshift and blueshift.
  • I can relate wavelength changes to motion.
  • I can describe how astronomers measure stellar motion.
  • I can explain the expansion of the universe using redshift.
  • I can compare Doppler effects for light and sound.

Doppler Effect for Light

The Doppler effect for light is a change in the observed wavelength and frequency of light caused by relative motion between a light source and an observer.

For light:

source moving away → longer observed wavelength → redshift

source moving toward observer → shorter observed wavelength → blueshift

Astronomers use these wavelength shifts to measure the motion of stars and galaxies. Redshift also provides some of the most important observational evidence that the universe is expanding.

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8

Light as an Electromagnetic Wave

Light is an electromagnetic wave.

Unlike sound, light does not require a material medium and can travel through a vacuum.

In a vacuum, all electromagnetic waves travel at:

c ≈ 3.00 × 10⁸ m/s

The relationship between speed, frequency, and wavelength is:

c = fλ

where:

c = speed of light

f = frequency

λ = wavelength

Therefore, frequency and wavelength are inversely related.

longer wavelength → lower frequency

shorter wavelength → higher frequency


Relative Motion and Light

Suppose a star and an observer are moving relative to one another.

If their separation is increasing, the observed light is shifted toward:

longer wavelengths

If their separation is decreasing, the observed light is shifted toward:

shorter wavelengths

These shifts are called:

redshift and blueshift


Redshift

Redshift occurs when observed light is shifted toward longer wavelengths.

For motion-related Doppler redshift, this occurs when a light source is:

moving away from the observer

The name comes from the visible spectrum, where red light has a longer wavelength than blue light.

Therefore:

receding source → wavelength increases → redshift

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8

Blueshift

Blueshift occurs when observed light is shifted toward shorter wavelengths.

For Doppler motion, this occurs when the source moves:

toward the observer

Therefore:

approaching source → wavelength decreases → blueshift

Blue and violet light have shorter wavelengths than red light.

The term "blueshift" therefore describes a shift toward the shorter-wavelength end of the visible spectrum.


Redshift and Blueshift Compared

Motion Observed Wavelength Observed Frequency Shift
Toward observer Shorter Higher Blueshift
Away from observer Longer Lower Redshift
No radial motion No Doppler change No Doppler change Neither

A useful memory rule is:

away → red

toward → blue


Does a Redshifted Star Actually Look Red?

Not necessarily.

Astronomers usually do not determine redshift simply by looking at the apparent colour of a star or galaxy.

Instead, they examine its:

spectrum

and look for recognizable spectral lines.

The positions of these lines can be measured extremely precisely.


Spectral Lines

Atoms and ions absorb or emit light at specific wavelengths.

These wavelengths produce recognizable patterns called:

spectral lines

Different elements have characteristic sets of spectral lines.

Examples include:

  • hydrogen
  • helium
  • sodium
  • calcium

These patterns act somewhat like fingerprints.

If astronomers know where a particular line should normally appear, they can compare it with where the line appears in light from a moving astronomical object.

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6

Measuring Redshift

Suppose a particular spectral line has a laboratory wavelength:

λ_rest = 500 nm

Astronomers observe the same identifiable line from a galaxy at:

λ_observed = 510 nm

The observed wavelength is longer.

Therefore, the line has shifted toward the red end of the spectrum.

The galaxy has:

redshift

For motion-related redshift, this indicates recession.


Measuring Blueshift

Suppose the same spectral line normally occurs at:

500 nm

but astronomers observe it at:

495 nm

The observed wavelength is shorter.

Therefore:

blueshift

This indicates motion toward the observer when the shift is caused by relative motion.


Rest Wavelength

The wavelength measured when there is no relative Doppler motion between source and observer is called the:

rest wavelength

It is often written:

λ₀

Astronomers compare the observed wavelength with this known value.

If:

λ_observed > λ₀

there is redshift.

If:

λ_observed < λ₀

there is blueshift.


Change in Wavelength

The wavelength change can be calculated using:

Δλ = λ_observed − λ₀

If Δλ is positive:

redshift

If Δλ is negative:

blueshift

This provides a simple numerical way to identify the direction of the shift.


Redshift Parameter

Astronomers often describe redshift using the quantity:

z = (λ_observed − λ₀)/λ₀

or:

z = Δλ/λ₀

The quantity z has no units.

If:

z > 0

the light is redshifted.

If:

z < 0

the light is blueshifted.


Worked Example: Calculating Redshift

A spectral line has a rest wavelength:

λ₀ = 600 nm

It is observed at:

λ_observed = 606 nm

First calculate:

Δλ = 606 − 600

Δλ = 6 nm

Then:

z = 6/600

z = 0.010

The positive value indicates:

redshift


Doppler Speed for Small Velocities

When an object's speed is much smaller than the speed of light, a useful approximation is:

v/c ≈ Δλ/λ₀

or:

v ≈ cz

This approximation works well for relatively small Doppler shifts.

It should not be used blindly for objects moving at speeds approaching the speed of light or for interpreting large cosmological redshifts.


Worked Example: Estimating Stellar Speed

Suppose:

z = 0.001

Using:

v ≈ cz

and:

c = 3.00 × 10⁸ m/s

v ≈ (3.00 × 10⁸)(0.001)

v ≈ 3.00 × 10⁵ m/s

or:

300 km/s

Because z is positive, this motion-related shift indicates recession.


Stellar Motion

Astronomers can use Doppler shifts to determine the radial velocity of stars.

Radial velocity means motion:

toward or away from the observer

If spectral lines are blueshifted:

star moving toward us

If spectral lines are redshifted:

star moving away from us

The greater the shift, the greater the radial speed in the simple low-speed Doppler model.


Radial vs Sideways Motion

The Doppler effect primarily reveals motion along the line of sight.

Imagine a star moving directly sideways across the sky.

Its distance from Earth may not be changing significantly at that instant.

Therefore, it may have:

little or no radial Doppler shift

Astronomers use other measurements to study sideways motion.

Thus, Doppler measurements reveal:

radial velocity

not necessarily the object's total velocity through space.


Measuring Stellar Motion

A simplified astronomical procedure is:

  1. Collect light from the star with a telescope.
  2. Separate the light into a spectrum.
  3. Identify known spectral lines.
  4. Measure their observed wavelengths.
  5. Compare them with laboratory rest wavelengths.
  6. Determine whether the lines are redshifted or blueshifted.
  7. Calculate the size of the shift.
  8. Use the shift to estimate radial velocity.

This allows motion to be measured even though the star may be trillions of kilometres away.


Detecting Binary Stars

Many stars orbit another star.

As one star moves around the system, it may alternately move:

toward Earth

and:

away from Earth

Its spectral lines therefore shift periodically:

blueshift → redshift → blueshift → redshift

This repeating pattern can reveal orbital motion.

Some binary systems can be detected this way even when telescopes cannot visually separate the two stars.


Detecting Exoplanets

A similar technique can help detect planets around other stars.

A planet does not simply orbit a perfectly stationary star.

The planet and star both orbit their common centre of mass.

As a result, the star makes a small repeating motion.

At one part of its motion:

star moves slightly toward Earth → blueshift

At another:

star moves slightly away → redshift

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6

The Radial Velocity Method

Astronomers measure the repeating shifts in the star's spectrum.

The pattern can provide information about:

  • orbital period
  • radial velocity of the star
  • evidence for an orbiting planet
  • a minimum estimate related to the planet's mass when combined with other information

This technique is called the:

radial velocity method

It has been extremely important in the discovery and study of exoplanets.


Redshift of Galaxies

When astronomers examine the spectra of many distant galaxies, they commonly find that their spectral features are shifted toward:

longer wavelengths

In other words, many distant galaxies show:

redshift

The systematic relationship between galaxy distance and redshift played a major role in establishing that the universe is expanding.

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9

Hubble's Observations

In the early twentieth century, observations showed an important relationship between galaxy distance and recession.

In the nearby universe, the relationship is approximately:

v = H₀d

where:

v = recession velocity

H₀ = Hubble constant

d = distance

This is known as the:

Hubble–Lemaître law

It indicates that more distant galaxies generally recede faster.


What Does an Expanding Universe Mean?

The expansion of the universe should not simply be pictured as galaxies flying outward from one central explosion point into empty space.

On large scales, it is better described as:

space itself expanding

As the universe expands, distances between widely separated, gravitationally unbound galaxies increase.

This expansion also stretches the wavelengths of light travelling through space.

The resulting wavelength increase is called:

cosmological redshift


Cosmological Redshift

For nearby objects and relatively small velocities, Doppler language provides a useful introduction.

However, the redshift of very distant galaxies is more accurately described as:

cosmological redshift

As the universe expands while light travels through it, the wavelength of the light is stretched.

Therefore:

expansion of space → wavelength increases → cosmological redshift

This is related to, but not exactly the same physical situation as, the ordinary Doppler effect from a source moving through space.


A Useful Expansion Model

Imagine dots drawn on the surface of an expanding balloon.

As the balloon expands:

  • distances between dots increase
  • each dot sees other distant dots moving farther away
  • there is no special central dot on the two-dimensional surface

This can help visualize cosmic expansion.

However, the balloon is only an analogy.

The universe is not necessarily expanding into a larger surrounding space in the way a balloon expands into a room.


Redshift and Distance

For relatively nearby galaxies following the Hubble flow:

greater distance → generally greater redshift

This does not mean every individual galaxy follows the relationship perfectly.

Galaxies also have local motions caused by gravity.

These are sometimes called:

peculiar velocities

For nearby galaxies, these local motions can noticeably affect the observed redshift or blueshift.


A Nearby Blueshifted Galaxy

Not every galaxy is redshifted.

Some nearby galaxies can move toward us because local gravitational motion is stronger than the expansion effect over that distance.

Such galaxies can show:

blueshift

This does not contradict the overall expansion of the universe.

The expansion relationship applies to the large-scale pattern.


Redshift as Evidence for Cosmic Expansion

Astronomers observe redshift in the spectra of large numbers of distant galaxies.

The general pattern is:

more distant galaxy → greater cosmological redshift

This supports the conclusion that the universe is expanding.

Redshift therefore provides important evidence for modern cosmological models.

It is not the only evidence, but it is one of the foundational observations.


Sound and Light: An Important Similarity

Both sound and light can show Doppler shifts.

For both:

approaching → higher observed frequency

receding → lower observed frequency

For sound:

higher frequency → higher pitch

lower frequency → lower pitch

For visible light:

higher frequency / shorter wavelength → blueshift

lower frequency / longer wavelength → redshift


Sound and Light: An Important Difference

Sound is a:

mechanical wave

It requires a medium such as:

  • air
  • water
  • solids

Light is an:

electromagnetic wave

It does not require a material medium and can travel through a vacuum.

This makes the physics of their Doppler effects different in important ways.


Moving Sources and Sound

For sound in still air, the medium provides a reference frame.

A moving sound source changes the spacing of wavefronts in the air.

Ahead:

compressed

Behind:

stretched

A moving observer instead changes how rapidly they encounter those wavefronts.

Therefore, moving-source and moving-observer cases have different classical sound equations.


Light Does Not Need a Medium

There is no equivalent stationary "light medium" like air for sound.

The speed of light in a vacuum is:

c

for all inertial observers.

Therefore, the Doppler effect for light must be described consistently with:

special relativity

At low relative speeds, the results resemble the familiar approaching/receding pattern from sound.

At speeds approaching c, relativistic effects become essential.


Comparing Sound and Light

Sound Doppler Effect Light Doppler Effect
Mechanical wave Electromagnetic wave
Requires a medium Does not require a medium
Approaching gives higher f Approaching gives higher f
Receding gives lower f Receding gives lower f
Higher f heard as higher pitch Higher f corresponds to shorter λ
Lower f heard as lower pitch Lower f corresponds to longer λ
Medium affects wave speed Travels at c in vacuum
Used with sirens and ultrasound Used extensively in astronomy

Frequency and Wavelength for Light

Because:

c = fλ

frequency and wavelength change in opposite directions.

For blueshift:

λ decreases

f increases

For redshift:

λ increases

f decreases

This is why redshift and blueshift can be described using either wavelength or frequency.

Astronomers commonly express the shift using wavelength.


Example: Predicting a Shift

A star is moving toward Earth.

No calculation is required.

Step 1:

Source is approaching.

Step 2:

Observed frequency increases.

Step 3:

Observed wavelength decreases.

Step 4:

The spectral lines move toward shorter wavelengths.

Therefore:

blueshift


Example: Receding Galaxy

A galaxy is receding.

Step 1:

Separation increases.

Step 2:

Observed wavelength becomes longer.

Step 3:

Spectral features move toward the red end of the spectrum.

Therefore:

redshift

For a distant galaxy participating in cosmic expansion, the more precise explanation is usually:

cosmological redshift


Worked Example: Identify the Motion

A hydrogen spectral line has a rest wavelength of:

656.3 nm

It is observed from a star at:

656.8 nm

Since:

656.8 nm > 656.3 nm

the wavelength has increased.

Therefore:

redshift

The star has a radial component of motion:

away from the observer

if the shift is interpreted as an ordinary motion-related Doppler shift.


Worked Example: Blueshift

A spectral line normally occurs at:

500.0 nm

It is observed at:

499.5 nm

Calculate:

Δλ = 499.5 − 500.0

Δλ = −0.5 nm

The negative change means the wavelength has decreased.

Therefore:

blueshift

The source is approaching along the line of sight.


Worked Example: Redshift Parameter

A galaxy has a spectral line with:

λ₀ = 400 nm

Observed wavelength:

λ_observed = 440 nm

Then:

z = (440 − 400)/400

z = 40/400

z = 0.10

The light is strongly redshifted.

For a shift this substantial, treating v = cz as an exact ordinary velocity relationship would not be appropriate.


Why Astronomers Use Spectra

A galaxy's overall colour can depend on many factors, including:

  • types of stars present
  • temperature
  • dust
  • star formation
  • chemical composition

Therefore, simply saying:

"That galaxy looks red, so it must be moving away"

would be unreliable.

Spectral lines provide identifiable wavelength markers.

Astronomers measure how these markers have shifted.


Spectroscopy

Spectroscopy is the study of spectra.

A spectroscope or spectrometer separates incoming light according to wavelength.

Spectroscopy can provide information about:

  • chemical composition
  • temperature
  • motion
  • density
  • magnetic fields
  • other physical conditions

Doppler shifts are therefore part of a much larger set of information contained in light.


Redshift Is Not Always Caused by Motion

It is important not to assume that every redshift has exactly the same cause.

Three important types include:

Doppler redshift

Associated with relative motion.

Cosmological redshift

Associated with the expansion of the universe.

Gravitational redshift

Associated with light moving through gravitational fields.

At this level, Doppler and cosmological redshift are the most important to distinguish.


Doppler Effect and the Expanding Universe

A useful progression is:

individual star

Doppler shift can reveal radial motion.

nearby galaxy

Spectral shift can reveal motion relative to us, including local gravitational motion.

distant galaxy

Large-scale redshift is interpreted in the context of cosmic expansion.

This prevents the oversimplification that all astronomical redshift is simply an ordinary source moving through stationary space.


Why Redshift Is So Useful

Astronomers cannot usually travel to stars or galaxies and directly measure their motion.

Instead, they analyze the light that reaches Earth.

From tiny shifts in wavelength, they can investigate:

  • stellar velocities
  • binary stars
  • exoplanets
  • galaxy motion
  • galaxy clusters
  • expansion of the universe

The wave properties of light therefore allow scientists to measure motion across enormous distances.


A Complete Stellar Example

A star produces hydrogen absorption lines.

One known line has:

λ₀ = 500 nm

Astronomers measure it at:

λ_observed = 501 nm

Since:

501 > 500

the wavelength has increased.

Therefore:

redshift

Calculate:

Δλ = 501 − 500

Δλ = 1 nm

Then:

z = 1/500

z = 0.002

For a relatively small shift:

v ≈ cz

v ≈ (3.00 × 10⁸)(0.002)

v ≈ 6.00 × 10⁵ m/s

or:

600 km/s

The positive motion-related shift indicates recession along the line of sight.


A Complete Universe Example

Astronomers observe many distant galaxies.

They identify known spectral lines.

Most of these distant galaxies show:

redshift

Furthermore, galaxies at greater distances generally show greater cosmological redshift.

This reveals a large-scale pattern in which distances between widely separated galaxies increase with time.

The evidence supports:

an expanding universe

The wavelength of light travelling across expanding space is also stretched.


A Reliable Strategy for Redshift and Blueshift Questions

  1. Identify the rest wavelength.
  2. Identify the observed wavelength.
  3. Compare them.
  4. If observed wavelength is longer, identify redshift.
  5. If observed wavelength is shorter, identify blueshift.
  6. For ordinary Doppler motion, redshift indicates recession.
  7. For ordinary Doppler motion, blueshift indicates approach.
  8. Calculate Δλ if required.
  9. Calculate z if required.
  10. For small Doppler shifts, use v ≈ cz if appropriate.
  11. Identify whether the question concerns a star, nearby galaxy, or cosmological expansion.
  12. Do not assume every redshift is simply an ordinary Doppler shift.
  13. Interpret the result in terms of radial motion or cosmic expansion as appropriate.

Common Mistakes

Thinking redshift means an object simply looks red

Astronomers usually measure shifts in spectral lines.

Thinking blueshift means a star must look blue

Blueshift refers to wavelengths shifting toward shorter values, not necessarily the overall visible colour.

Reversing redshift and blueshift

Away → redshift. Toward → blueshift.

Thinking wavelength and frequency both increase

Because c = fλ, increasing wavelength corresponds to decreasing frequency in vacuum.

Thinking Doppler measurements reveal all of an object's motion

They primarily reveal radial motion along the line of sight.

Thinking sound and light require the same medium

Sound requires a material medium. Light does not.

Thinking light behaves exactly like sound for moving sources

The qualitative approaching/receding pattern is similar, but the detailed physics of light requires relativity.

Using v = cz for every redshift

This is a useful low-redshift approximation, not a universal velocity equation.

Thinking all astronomical redshift has exactly the same cause

Doppler, cosmological, and gravitational redshifts are distinct phenomena.

Thinking galaxies are simply flying outward from one central point

Cosmic expansion is better understood as increasing distances caused by the expansion of space on large scales.


Key Terms

Doppler effect — change in observed frequency or wavelength associated with relative motion.

Electromagnetic wave — oscillating electric and magnetic fields capable of travelling through a vacuum.

Redshift — shift of observed light toward longer wavelengths.

Blueshift — shift of observed light toward shorter wavelengths.

Rest wavelength (λ₀) — wavelength measured without the relevant Doppler shift.

Observed wavelength — wavelength measured by the observer.

Spectral line — identifiable wavelength feature produced by emission or absorption.

Spectrum — distribution of electromagnetic radiation according to wavelength or frequency.

Spectroscopy — study and measurement of spectra.

Radial velocity — component of velocity toward or away from an observer.

Redshift parameter (z) — fractional change in wavelength, z = Δλ/λ₀.

Hubble–Lemaître law — approximate relationship between distance and recession rate for galaxies in the nearby expanding universe.

Hubble constant (H₀) — proportionality constant in the Hubble–Lemaître relationship.

Cosmological redshift — increase in observed wavelength associated with the expansion of the universe while light travels through space.

Gravitational redshift — wavelength increase associated with gravitational effects.

Binary star — system containing two stars orbiting a common centre of mass.

Exoplanet — planet orbiting a star outside our Solar System.

Radial velocity method — technique that detects periodic stellar spectral shifts caused by orbital motion associated with an orbiting companion.


Key Takeaways

  • Light can undergo a Doppler shift.
  • Light approaching an observer is shifted toward shorter wavelengths.
  • Shorter-wavelength motion-related shifts are called blueshift.
  • Light from a receding source is shifted toward longer wavelengths.
  • Longer-wavelength motion-related shifts are called redshift.
  • Blueshift corresponds to higher observed frequency.
  • Redshift corresponds to lower observed frequency.
  • Astronomers usually measure shifts in spectral lines rather than simply looking at an object's colour.
  • Spectral lines provide known wavelength markers.
  • Comparing observed and rest wavelengths reveals the direction of a shift.
  • Redshift can indicate radial motion away from an observer.
  • Blueshift can indicate radial motion toward an observer.
  • Doppler measurements primarily reveal radial velocity rather than total space velocity.
  • Repeating redshift and blueshift can reveal orbital motion.
  • The radial velocity method can help detect exoplanets.
  • Most sufficiently distant galaxies show cosmological redshift.
  • Greater distance is generally associated with greater cosmological redshift on large scales.
  • These observations support the conclusion that the universe is expanding.
  • Cosmic expansion is better described as the expansion of space rather than galaxies exploding outward from a central point.
  • Cosmological redshift is related to but physically distinct from the simple classical Doppler effect.
  • Sound requires a material medium, while light does not.
  • Both sound and light show higher observed frequency for approach and lower observed frequency for recession.
  • Sound Doppler shifts can be heard as pitch changes.
  • Light Doppler shifts are measured as changes in wavelength or frequency.
  • Precise light Doppler physics at high relative speeds requires special relativity.
  • Understanding redshift allows astronomers to investigate motion and the structure and evolution of the universe.

Check Your Understanding

  1. Define redshift and blueshift.
  2. A star is moving toward Earth. Predict whether its spectral lines will be redshifted or blueshifted.
  3. A galaxy's spectral lines are shifted toward longer wavelengths. What type of shift has occurred?
  4. Explain the relationship between wavelength and frequency for light using c = fλ.
  5. A spectral line has a rest wavelength of 500 nm but is observed at 505 nm. Identify the shift and describe the motion it would indicate if caused by the ordinary Doppler effect.
  6. A spectral line normally occurs at 650 nm but is observed at 648 nm. Is this redshift or blueshift? What does it indicate about radial motion?
  7. Calculate the redshift parameter z for a line with λ₀ = 600 nm and λ_observed = 603 nm.
  8. Explain how astronomers use spectral lines to determine whether a star is moving toward or away from Earth.
  9. Why is simply looking at whether a galaxy appears red or blue not a reliable method for measuring Doppler shift?
  10. Explain what radial velocity means and why Doppler measurements do not necessarily reveal an object's complete velocity through space.
  11. Describe how repeating redshift and blueshift of a star can provide evidence for an orbiting planet.
  12. Explain how observations of distant galaxy redshifts support the idea that the universe is expanding.
  13. Distinguish between an ordinary Doppler redshift and cosmological redshift.
  14. Compare the Doppler effect for sound and light. Include at least two similarities and two differences.
  15. A student says, "Distant galaxies are redshifted because they are all flying through space away from one central point, exactly like the lower pitch of an ambulance driving away." Evaluate this statement. Explain what the analogy gets right, what it oversimplifies, and how cosmic expansion provides a more accurate description.
 
 
 

5. Applications of the Doppler Effect

Learning outcomes
  • I can describe medical ultrasound Doppler imaging.
  • I can explain radar speed detection.
  • I can describe weather radar applications.
  • I can identify astronomical applications.
  • I can explain how Doppler measurements are used in modern science and technology.

Applications of the Doppler Effect

The Doppler effect is the change in observed frequency or wavelength caused by relative motion between a wave source and an observer.

This effect is much more than the familiar change in pitch of a passing siren. Scientists and engineers use Doppler measurements to determine the motion of objects that may be difficult, dangerous, extremely small, or extremely distant to measure directly.

Important applications include:

  • medical ultrasound
  • radar speed detection
  • weather radar
  • aviation and navigation
  • astronomy
  • satellite measurements
  • industrial monitoring

In many of these applications, motion is converted into a measurable frequency shift.

https://images.openai.com/static-rsc-4/9ND5KbTEH4pJtM61UTHKGVPix7S1UrtW8gltFHROfQyHYyy9r90fPwTK5YvqSepDJXRgJRljAFJ9j_1eE7AKTWDRni1I-M321MuvCOWv1IefNE_tQ2G-BwE7-7E6XUrJwM1uXwT75qS7PrEWdqZwma5KHaqR4BMmbPpKDDKaMtNnGijjORBSzqqeMChUIUCz?purpose=fullsize
 

The Basic Measurement Principle

A Doppler system usually compares two frequencies:

transmitted or emitted frequency

and

received or observed frequency

If the reflecting object or source is moving, these frequencies can differ.

The difference is called the:

Doppler shift

A simplified expression is:

Δf = f_observed − f_emitted

The direction and size of this shift provide information about motion.


What Doppler Measurements Tell Us

Doppler measurements can provide information about:

  • whether something is approaching or receding
  • radial speed
  • direction of fluid flow
  • movement inside the human body
  • vehicle speed
  • wind motion
  • storm rotation
  • stellar motion
  • galaxy motion
  • orbital motion

The important quantity is usually the component of velocity:

toward or away from the detector

This is called radial velocity.


Doppler Ultrasound

Doppler ultrasound is a medical technique that uses high-frequency sound waves to investigate moving structures inside the body.

It is especially useful for studying:

blood flow

Ultrasound waves are transmitted into the body by a device called a:

transducer

The sound interacts with moving blood cells, and some of the ultrasound returns to the transducer.

The frequency of the returning sound depends on the motion of the blood.

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7

How Doppler Ultrasound Works

A simplified sequence is:

  1. The transducer produces ultrasound.
  2. Ultrasound travels into the body.
  3. The waves encounter moving blood cells.
  4. Some ultrasound is scattered or reflected back toward the transducer.
  5. Motion of the blood cells causes a Doppler frequency shift.
  6. The transducer detects the returning ultrasound.
  7. A computer analyzes the frequency shift.
  8. Information about blood flow is produced.

The system therefore turns an invisible movement inside the body into measurable wave information.


Blood Moving Toward the Transducer

If blood cells have a velocity component toward the ultrasound transducer, the returning ultrasound undergoes a Doppler shift corresponding to:

higher received frequency

The equipment can recognize this shift and determine the direction of flow.


Blood Moving Away from the Transducer

If blood cells have a velocity component away from the transducer:

received frequency decreases

Therefore:

toward transducer → higher frequency

away from transducer → lower frequency

The equipment can use both the direction and magnitude of the shift.


Doppler Ultrasound and Blood Speed

The larger the relevant Doppler frequency shift, the larger the radial component of blood velocity, all else being equal.

However, the measurement also depends on the angle between:

  • the ultrasound beam
  • the direction of blood flow

This means probe position matters.

Doppler ultrasound does not simply measure all motion equally well in every direction.


Why the Beam Angle Matters

Doppler ultrasound measures motion most effectively when blood has a substantial velocity component along the ultrasound beam.

If blood moves almost directly toward or away from the transducer:

strong radial component

If blood moves perpendicular to the beam:

very small radial component

Therefore, the Doppler shift becomes small when motion is close to perpendicular to the ultrasound beam.


Colour Doppler Imaging

Colour Doppler combines conventional ultrasound imaging with Doppler measurements.

The ultrasound image shows body structures.

Colour information is added to represent blood-flow information such as:

  • direction
  • relative velocity

The colours are assigned by the imaging system.

They do not represent the actual colour of blood.

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8

Interpreting Colour Doppler

A common convention displays flow toward the transducer with one colour and flow away with another.

However:

the exact colour convention depends on the machine settings.

Therefore, it is better to interpret the displayed scale than to memorize that one particular colour always means toward or away.

The important physics is:

direction of motion → direction of frequency shift


Medical Applications of Doppler Ultrasound

Doppler ultrasound can be used to investigate:

  • blood flow through arteries
  • blood flow through veins
  • heart function
  • heart valves
  • circulation
  • narrowed blood vessels
  • abnormal flow patterns
  • fetal and placental circulation in appropriate clinical settings

It provides useful information without requiring surgery.


Doppler Echocardiography

An echocardiogram uses ultrasound to study the heart.

Doppler techniques can be added to investigate blood movement through:

  • heart chambers
  • heart valves
  • major vessels

Doctors can use this information alongside other measurements to evaluate heart function.


Advantages of Doppler Ultrasound

Doppler ultrasound has several practical advantages.

It can:

  • measure motion inside the body
  • provide information in real time
  • produce images without ionizing radiation
  • be repeated when medically appropriate
  • combine structural imaging with flow measurements

This makes Doppler physics extremely valuable in modern medicine.


Radar Speed Detection

The Doppler effect can also be used with:

electromagnetic waves

Radar speed systems transmit electromagnetic radiation toward a moving vehicle.

The waves reflect from the vehicle and return to the radar detector.

Because the vehicle is moving, the returning waves have a slightly different frequency.

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4

How Radar Measures Speed

A simplified radar-speed measurement works like this:

  1. Radar transmits a known frequency.
  2. The electromagnetic wave travels toward a vehicle.
  3. The wave reflects from the vehicle.
  4. The reflected wave returns to the radar.
  5. The returning frequency is measured.
  6. The frequency shift is calculated.
  7. The shift is converted into a radial speed.

Therefore:

motion → Doppler shift → calculated speed


Vehicle Moving Toward Radar

If a vehicle moves toward the radar detector:

received frequency increases

The returning wave is Doppler shifted upward.

A larger shift generally corresponds to a greater radial speed.


Vehicle Moving Away from Radar

If the vehicle moves away:

received frequency decreases

The direction of the frequency shift therefore helps identify whether the target is approaching or receding.


Radar Measures Radial Speed

Suppose a car travels directly toward a radar unit.

Almost all its velocity is radial.

The radar can obtain a strong measurement of its speed toward the detector.

Now suppose the car travels mostly sideways across the detector's field of view.

Only part of its velocity is toward or away from the radar.

Therefore, Doppler radar fundamentally measures:

radial velocity

rather than automatically measuring the complete velocity vector.


Angle and Radar Measurements

Suppose a vehicle travels at speed v at an angle θ to the radar's line of sight.

The radial component is:

v_radial = v cos θ

If θ = 0°:

v_radial = v

If θ becomes larger:

v_radial becomes smaller

At 90°:

cos 90° = 0

so the radial component is zero.

This demonstrates why detector geometry matters.


Conceptual Radar Example

Car A moves directly toward a radar unit at 20 m/s.

Car B moves at the same speed but mostly sideways across the detector's view.

Which produces the larger Doppler shift?

Car A

because more of its velocity is directed toward the radar.

This is a useful reminder that Doppler systems measure motion along the line of sight.


Why Electromagnetic Waves Are Useful for Radar

Radar waves travel at approximately:

3.00 × 10⁸ m/s

in air.

They can:

  • travel rapidly over large distances
  • reflect from many objects
  • be generated at precise frequencies
  • be detected electronically
  • carry detailed information

Small frequency shifts can be measured electronically with high precision.


Weather Radar

Weather radar sends electromagnetic waves into the atmosphere.

These waves interact with precipitation particles such as:

  • raindrops
  • snowflakes
  • ice particles
  • hail

Some of the electromagnetic energy returns to the radar.

The returning signal provides information about the atmosphere.

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8

Reflection and Doppler Shift in Weather Radar

Weather radar uses two important ideas.

Reflection and scattering

provide information about where precipitation is located and aspects of its intensity.

Doppler shift

provides information about radial motion.

The radar therefore obtains information about both:

where precipitation is

and

how targets are moving toward or away from the radar


Precipitation Moving Toward Radar

If precipitation has a velocity component toward the radar:

returned frequency is shifted upward

This indicates motion toward the detector.


Precipitation Moving Away

If precipitation moves away:

returned frequency is shifted downward

Meteorologists can map these different radial velocities across a storm.


Detecting Storm Rotation

Suppose one part of a storm shows motion toward the radar while a nearby region shows motion away.

This pattern can indicate:

rotation

Meteorologists analyze these velocity patterns to identify potentially dangerous storm structures.

Doppler radar can therefore contribute to:

  • severe-weather monitoring
  • thunderstorm analysis
  • tornado detection and warning
  • wind studies

What Weather Radar Actually Measures

Weather radar does not directly measure every part of the wind velocity.

It measures:

motion toward or away from the radar

Therefore, meteorologists must interpret the pattern across many radar measurements.

The observed motion of precipitation particles is used as information about atmospheric motion.


Weather Radar and Rainfall

Radar return strength can also provide information related to precipitation.

A stronger returned signal may indicate a greater amount or different type of reflecting material, although interpretation depends on many factors.

Therefore, weather radar can help estimate:

  • location of precipitation
  • movement of precipitation
  • storm structure
  • rainfall patterns
  • hail regions

Doppler velocity adds motion information to these observations.


Aviation Applications

Doppler and radar technologies are important in aviation.

They can contribute to:

  • weather monitoring
  • aircraft tracking
  • wind measurement
  • navigation
  • detection of hazardous atmospheric conditions

Pilots and air-traffic systems depend on wave-based measurements to improve safety.


Astronomy

Astronomy provides some of the most remarkable Doppler applications.

Astronomers cannot place speed sensors directly on distant stars.

Instead, they analyze:

light

The wavelengths of identifiable spectral lines can reveal motion toward or away from Earth.

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8

Spectral Lines

Atoms produce characteristic patterns of spectral lines.

Astronomers know the normal or:

rest wavelengths

of many of these lines.

They compare those values with the wavelengths observed from a star.

If the lines shift toward shorter wavelengths:

blueshift

If the lines shift toward longer wavelengths:

redshift


Measuring Stellar Motion

For ordinary motion-related Doppler shifts:

blueshift → star has motion toward us

redshift → star has motion away from us

The amount of shift can be used to calculate:

radial velocity

This allows astronomers to measure motion across enormous distances.


Detecting Binary Stars

Two stars can orbit their common centre of mass.

As a star moves around its orbit, it may alternately move:

  • toward Earth
  • away from Earth

Its spectral lines therefore shift:

blue → red → blue → red

in a repeating pattern.

Astronomers can use this pattern to identify and study:

binary star systems

even when the stars are difficult to separate visually.


Detecting Exoplanets

Planets can also be detected using Doppler measurements.

A star and planet both orbit their common centre of mass.

The star therefore makes a small repeating motion.

When the star moves slightly toward Earth:

spectral lines blueshift

When it moves slightly away:

spectral lines redshift

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6

The Radial Velocity Method

This technique is called the:

radial velocity method

Astronomers repeatedly measure a star's spectrum.

They look for a periodic pattern in its radial velocity.

From the pattern they can obtain information about:

  • orbital period
  • stellar motion
  • evidence for an orbiting planet
  • properties of the orbit
  • constraints on the planet's mass

This demonstrates the extraordinary precision possible with modern Doppler measurements.


Galaxy Motion

Spectral shifts are also used to study galaxies.

For motion-related shifts:

redshift → recession

blueshift → approach

Nearby galaxies can have motions caused by gravitational interactions.

At much larger scales, the widespread redshift of distant galaxies is connected to:

cosmic expansion


Expansion of the Universe

Astronomers observe that sufficiently distant galaxies generally show:

redshift

The large-scale relationship between distance and recession is described approximately in the nearby universe by:

v = H₀d

where:

v = recession velocity

H₀ = Hubble constant

d = distance

This relationship is known as the:

Hubble–Lemaître law


Cosmological Redshift

For very distant galaxies, it is more accurate to describe the observed shift as:

cosmological redshift

As the universe expands, the wavelength of light travelling through space is stretched.

Therefore:

expansion of space → longer observed wavelength → redshift

This is related to the Doppler ideas used for ordinary motion but is not exactly the same physical phenomenon as a siren moving through air.


Measuring Rotation of Galaxies

Doppler measurements can also reveal rotation.

Imagine a rotating galaxy.

One side may rotate partly toward Earth.

That side can show:

blueshift

The opposite side may rotate partly away.

That side can show:

redshift

By measuring these shifts across a galaxy, astronomers can study its rotation.


Measuring the Sun's Rotation

The same principle can be applied to the Sun.

One edge of the rotating Sun has a component of motion toward Earth.

The opposite edge has a component away.

Tiny shifts in spectral lines can therefore provide information about:

solar rotation

Doppler measurements allow scientists to study motion without physically touching the object.


Measuring Motion in Stars

Spectral-line shifts can also reveal motions on and within stellar atmospheres.

Scientists can investigate:

  • rotation
  • pulsation
  • atmospheric motion
  • orbital motion

The ability to measure tiny wavelength shifts makes spectroscopy one of astronomy's most powerful tools.


Doppler Measurements in Satellites and Spacecraft

Radio communication with spacecraft can also contain Doppler information.

If a spacecraft moves relative to Earth, the received radio frequency can shift.

Careful measurements can help scientists investigate:

  • spacecraft velocity
  • orbital motion
  • trajectory changes

Extremely precise radio-frequency measurements can therefore support spacecraft navigation and scientific experiments.


Industrial Applications

Doppler measurement techniques are also used in engineering and industry.

Possible applications include measuring:

  • fluid flow
  • vibration
  • rotating machinery
  • surface motion
  • particle motion

Because Doppler methods can often make measurements without direct mechanical contact, they can be useful in situations involving:

  • high temperatures
  • dangerous machinery
  • delicate surfaces
  • rapidly moving objects

Laser Doppler Measurements

Light can be used instead of sound or microwaves.

A laser beam can interact with a moving surface or moving particles.

The returned or scattered light may contain a Doppler frequency shift.

This principle can be used in instruments that measure:

  • vibration
  • fluid velocity
  • surface velocity

These systems demonstrate that the same underlying wave principle can operate across very different technologies.


Comparing Major Doppler Applications

Application Wave Used Moving Target Information Obtained
Medical Doppler Ultrasound Blood cells Blood-flow direction and velocity
Speed radar Electromagnetic waves Vehicle Radial speed
Weather radar Electromagnetic waves Precipitation Radial motion and storm structure
Stellar spectroscopy Light Star Radial velocity
Exoplanet detection Light Star Periodic stellar motion
Galaxy studies Light Stars/galaxies Motion and cosmic redshift
Spacecraft tracking Radio waves Spacecraft Radial motion
Laser Doppler systems Light Surfaces/particles Velocity or vibration

Different Waves, Same Basic Idea

The technologies may look very different.

A doctor examining blood flow and an astronomer observing a star appear to be doing completely different things.

But both can use the same fundamental idea:

motion causes a measurable frequency shift

The wave might be:

  • sound
  • radio
  • microwave
  • visible light

The scale might range from:

blood cells → vehicles → storms → stars → galaxies

Yet the underlying wave principle remains closely related.


Why Frequency Is So Useful

Frequency can be measured very precisely.

Electronic and optical instruments can detect changes far too small for humans to notice directly.

This means Doppler techniques can detect very small motions.

For example:

  • tiny stellar movements may reveal a planet
  • small blood-flow changes can be measured medically
  • atmospheric motion can be mapped remotely
  • spacecraft motion can be tracked over enormous distances

Remote Measurement

One major advantage of Doppler technology is that it can measure motion:

remotely

The detector does not necessarily need physical contact with the moving object.

Instead:

  1. a wave is emitted or received
  2. the frequency is measured
  3. the shift is determined
  4. motion is calculated

This is particularly useful when the target is:

  • inside the human body
  • moving rapidly
  • dangerous to approach
  • high in the atmosphere
  • in space
  • extremely distant

Non-Invasive Measurement

In medicine, Doppler ultrasound provides a particularly important advantage:

non-invasive measurement

Doctors can obtain information about blood flow without inserting a mechanical speed sensor into the vessel.

Similarly, astronomers can determine the motion of a star without travelling anywhere near it.

Wave behaviour allows information to be gathered from a distance.


Doppler Shift and Radial Velocity

One limitation appears in nearly every Doppler application.

The Doppler effect primarily measures:

radial velocity

This is the velocity component along the line connecting the object and detector.

Therefore:

directly toward detector → large approaching shift

directly away → large receding shift

sideways → small or zero ordinary radial shift

Understanding this limitation is essential when interpreting Doppler measurements.


The Angle Problem

Suppose an object moves at:

v = 30 m/s

at an angle of 60° to the detector's line of sight.

The radial velocity is:

v_radial = v cos θ

v_radial = 30 cos 60°

v_radial = 30 × 0.5

v_radial = 15 m/s

Although the object's actual speed is 30 m/s, the Doppler measurement corresponds to a radial component of:

15 m/s

This principle matters in radar, ultrasound, astronomy, and many other applications.


Worked Example: Radar Interpretation

A radar unit detects a vehicle producing a Doppler shift corresponding to:

25 m/s toward the detector

What does this directly tell us?

It tells us the vehicle has a:

25 m/s radial velocity toward the radar

If the vehicle is moving directly toward the radar, its speed is approximately 25 m/s.

If it is travelling at an angle, its actual speed can be greater.


Worked Example: Medical Interpretation

A Doppler ultrasound system detects blood moving toward the transducer.

The returned ultrasound has a frequency higher than the transmitted frequency.

Therefore:

positive approaching Doppler shift

If the blood changes direction and moves away:

the direction of the frequency shift reverses

The system can use this information to map blood-flow direction.


Worked Example: Astronomy

A known spectral line has:

λ₀ = 500 nm

It is observed from a star at:

λ_observed = 500.5 nm

Since:

500.5 > 500

the wavelength has increased.

Therefore:

redshift

For an ordinary motion-related Doppler interpretation, the star has a radial component of motion:

away from Earth


Worked Example: Weather Radar

A storm contains two nearby regions.

Region A contains precipitation moving toward the radar.

Region B contains precipitation moving away.

The radar detects:

Region A → approaching Doppler shift

Region B → receding Doppler shift

A nearby pair of opposite radial velocities can be an important clue that the storm contains:

rotation

Meteorologists then analyze the complete radar pattern and other observations to assess the storm.


Doppler Measurements and Modern Computing

Modern Doppler systems do more than detect a single frequency.

Computers can process large numbers of signals rapidly.

This allows systems to create:

  • blood-flow maps
  • storm velocity maps
  • vehicle-speed readings
  • stellar radial-velocity curves
  • three-dimensional scientific models

Improved electronics and computing have made Doppler measurements increasingly precise and useful.


Combining Doppler with Other Measurements

Doppler data is often most powerful when combined with other information.

For example:

Medical imaging

Doppler flow + structural ultrasound image

Weather forecasting

Doppler velocity + precipitation radar + satellite observations

Astronomy

Radial velocity + transit observations + imaging

Vehicle systems

Doppler radar + cameras + other sensors

One measurement technique rarely provides every piece of information needed.


Advantages of Doppler Technology

Doppler techniques can be:

  • remote
  • rapid
  • precise
  • non-contact
  • non-invasive in medical applications
  • useful for real-time monitoring
  • applicable over enormous ranges of distance

The same physics can therefore be adapted to many different scientific problems.


Limitations of Doppler Measurements

Doppler measurements also have limitations.

They may be affected by:

  • measurement angle
  • signal noise
  • reflections
  • interference
  • weak returned signals
  • complex motion
  • instrument resolution
  • assumptions used in calculations

Most importantly:

Doppler measurements primarily reveal radial motion.

Scientists and engineers must interpret the measurements carefully.


Evaluating Doppler Technology

A good evaluation should consider both benefits and limitations.

For example:

Doppler ultrasound

Benefit: non-invasive measurement of blood flow.

Limitation: measurement depends on beam angle and signal quality.

Radar

Benefit: remote measurement of vehicle or atmospheric motion.

Limitation: primarily measures radial velocity.

Astronomical spectroscopy

Benefit: measures motion across enormous distances.

Limitation: directly measures only the line-of-sight component of velocity.

Understanding the physics allows scientists to recognize and compensate for these limitations.


From Blood Cells to Galaxies

The range of Doppler applications is extraordinary.

At the small scale:

moving blood cells

can create measurable Doppler shifts.

At the human scale:

moving vehicles

can be measured.

At the atmospheric scale:

storms

can be monitored.

At the planetary scale:

spacecraft

can be tracked.

At the astronomical scale:

stars and galaxies

can be studied.

The same basic wave principle connects all of these technologies.


A Reliable Strategy for Doppler Application Questions

When analyzing a Doppler application:

  1. Identify the wave being used.
  2. Identify the source.
  3. Identify the observer or detector.
  4. Identify what is moving.
  5. Determine whether the motion is toward or away from the detector.
  6. Predict whether the observed frequency increases or decreases.
  7. Identify the Doppler shift.
  8. Determine what information the shift provides.
  9. Consider the radial component of velocity.
  10. Consider whether the measurement angle matters.
  11. Identify the practical purpose of the technology.
  12. Identify at least one advantage.
  13. Identify at least one limitation.
  14. Explain how the measurement improves scientific or technological understanding.

Common Mistakes

Thinking Doppler ultrasound simply produces a picture

Conventional ultrasound provides structural imaging, while Doppler techniques specifically provide information about motion and flow.

Thinking Doppler ultrasound uses electromagnetic radiation

Ultrasound is a mechanical sound wave.

Thinking colour Doppler shows the real colour of blood

The colours are computer-generated representations of flow information.

Memorizing one Doppler colour convention

Colour assignments can depend on equipment settings. Always check the displayed scale.

Thinking radar directly measures every component of vehicle velocity

Doppler radar fundamentally measures radial motion.

Thinking weather radar directly measures all wind

It measures radial motion of targets such as precipitation, which meteorologists use to infer atmospheric motion.

Thinking redshift always means ordinary Doppler motion

Distant-galaxy redshift is more accurately interpreted using cosmological expansion.

Thinking a star must visibly change colour

Astronomers measure tiny shifts in spectral lines.

Ignoring measurement angle

Doppler measurements depend strongly on the component of motion along the detector's line of sight.

Thinking a larger frequency shift always means a faster total speed

It directly indicates a larger radial component, assuming the other relevant conditions are unchanged.

Thinking Doppler techniques require physical contact

One of their major advantages is the ability to measure motion remotely.


Key Terms

Doppler effect — change in observed frequency or wavelength associated with relative motion.

Doppler shift — difference between transmitted or emitted frequency and received frequency.

Radial velocity — velocity component toward or away from an observer.

Ultrasound — sound with frequency above the normal human hearing range.

Doppler ultrasound — technique using ultrasound frequency shifts to investigate moving structures or fluids.

Transducer — device that produces and detects ultrasound.

Colour Doppler — ultrasound technique displaying flow information using computer-assigned colours.

Echocardiography — ultrasound examination of the heart.

Radar — system using electromagnetic waves to detect objects and obtain information about their location or motion.

Doppler radar — radar that uses frequency shifts to measure radial motion.

Weather radar — radar system used to detect and analyze atmospheric targets such as precipitation.

Spectral line — identifiable wavelength feature produced by emission or absorption.

Redshift — shift toward longer wavelengths.

Blueshift — shift toward shorter wavelengths.

Radial velocity method — astronomical technique using periodic Doppler shifts to investigate orbital motion and detect companions such as exoplanets.

Cosmological redshift — wavelength increase associated with the expansion of the universe.

Laser Doppler measurement — use of Doppler shifts in light to determine motion or velocity.

Non-invasive — obtaining information without entering or significantly damaging the body.

Non-contact measurement — measurement made without physically attaching a sensor to the moving object.


Key Takeaways

  • Doppler measurements convert motion into measurable changes in frequency or wavelength.
  • Doppler ultrasound uses sound waves to investigate blood flow.
  • Moving blood cells cause frequency shifts in returning ultrasound.
  • Blood moving toward a transducer and blood moving away produce opposite Doppler shifts.
  • Colour Doppler uses computer-assigned colours to represent flow information.
  • Doppler ultrasound can provide real-time, non-invasive information about circulation.
  • Radar speed detection uses electromagnetic waves reflected from moving vehicles.
  • The returning radar frequency changes because of the vehicle's motion.
  • Doppler radar primarily measures radial velocity.
  • Measurement angle affects the radial component detected.
  • Weather radar uses returned electromagnetic waves to investigate precipitation and atmospheric motion.
  • Opposing radial velocities in nearby regions can provide evidence of storm rotation.
  • Doppler weather radar contributes to severe-weather monitoring.
  • Astronomers measure shifts in spectral lines to determine stellar radial motion.
  • Blueshift can indicate motion toward the observer.
  • Redshift can indicate motion away when caused by ordinary relative motion.
  • Repeating stellar Doppler shifts can reveal binary stars.
  • Small periodic Doppler shifts can provide evidence for exoplanets.
  • Doppler measurements can reveal rotation in stars and galaxies.
  • Cosmological redshift helps scientists investigate the expansion of the universe.
  • Spacecraft radio signals can contain Doppler information useful for tracking motion.
  • Laser Doppler techniques can measure fluid flow, vibration, and surface velocity.
  • Doppler techniques can make measurements without direct physical contact.
  • Doppler measurements usually provide the component of velocity along the line of sight rather than the complete velocity.
  • Modern computers allow Doppler measurements to be converted into detailed images, maps, and motion data.
  • Doppler technology connects medicine, transportation, meteorology, engineering, space exploration, and astronomy through the same fundamental wave principle.

Check Your Understanding

  1. Explain the basic principle that allows the Doppler effect to be used to measure motion.
  2. Describe how Doppler ultrasound can measure blood flow.
  3. What happens to the received ultrasound frequency when blood moves toward the transducer?
  4. Why does the angle between an ultrasound beam and blood flow affect a Doppler measurement?
  5. Explain why colour Doppler images do not show the actual colour of blood.
  6. Describe how a radar speed detector uses the Doppler effect to measure a vehicle's motion.
  7. A vehicle moves directly toward a radar detector. Predict what happens to the frequency of the returned radar signal.
  8. A vehicle travels at 30 m/s at an angle of 60° to the radar's line of sight. Calculate its radial velocity using v_radial = v cos θ.
  9. Explain how Doppler weather radar obtains information about motion within a storm.
  10. Why might nearby regions showing motion toward and away from a weather radar provide evidence of storm rotation?
  11. Describe how astronomers use spectral lines to measure the radial velocity of a star.
  12. Explain how periodic redshift and blueshift can provide evidence for an orbiting exoplanet.
  13. Give one similarity and one difference between Doppler ultrasound, vehicle radar, and astronomical Doppler measurements.
  14. Explain why Doppler measurements generally provide radial velocity rather than the complete velocity of an object.
  15. Evaluate the statement: "The Doppler effect is useful because the same basic wave principle allows scientists to measure motion ranging from blood cells inside the human body to stars and galaxies across the universe." Support your answer with at least three technological or scientific applications.