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Waves & Sound

The Doppler Effect

The siren never changes its note. The pitch you hear changes because each crest starts from a different place.

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The Doppler Effect

The siren never changes its note. The pitch you hear changes because each crest starts from a different place.

35 min3 checkpoints9 simulation tasks

Introduction

An ambulance goes past and the siren drops in pitch, though it plays one note the whole time.

Predict

A car with its horn stuck on drives straight at you at constant speed. You stand in the middle of the road. What do you hear before it reaches you?

Head on

Read the graph

The horn plays 60 Hz and drives straight at the listener at 120 m/s. Run it. What pitch does the listener hear while it approaches?

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Run the simulation first, then read the value off it.

The source makes a crest, and that crest at once loses all connection with the source. It spreads as a circle centred on the spot where it was made, at the speed of the air. Meanwhile the source moves on and makes the next one somewhere else.

Where each crest is born

Try it

Parked, the horn sends out crests 5.72 m apart. Set its speed so the crests ahead of it are packed half as far apart.

GoalCrests ahead of the horn half as far apart: 2.86 m.

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Each circle is centred where the source was when it was emitted, and grows at the speed of sound vv. In one period the source advances vsT0v_s T_0 while its last crest advances vT0v T_0, so the gap ahead is short by the distance the source covered:

λ+=v−vsf0and behind itλ−=v+vsf0\lambda_+ = \frac{v - v_s}{f_0} \qquad\text{and behind it}\qquad \lambda_- = \frac{v + v_s}{f_0}
Practice

The source in the simulation is closing on the observer at 120 m/s. How fast is the sound from it moving through the air toward the observer?

Try it

Make the sound from this horn cross the air faster than 350 m/s.

GoalSound crossing the air faster than 350 m/s.

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The frequency an observer hears

Crests reach the observer λ±/v\lambda_\pm / v seconds apart, so the heard frequency is v/λ±v/\lambda_\pm. For a source and an observer both moving along the line joining them,

f=f0 v+vov−vsf = f_0\,\frac{\vel{v} + \vel{v_o}}{\vel{v} - \vel{v_s}}

with vsv_s positive when the source moves toward the observer and vov_o positive when the observer moves toward the source.


Try it

The horn is parked 120 m up the road to your left, playing 60 Hz. Walk toward it fast enough to hear it above 66 Hz, and run it.

GoalHear the parked horn above 66 Hz.

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Try it

Now you stand still and the horn drives at you. Set its speed so that, as it approaches, you hear 1.5 times the note it plays. Then run it.

GoalHear 90 Hz, 1.5 times the horn's note, as it approaches.

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Passing beside you

Try it

Run the head-on pass. Then move the listener 40 m or more to the side of the road and run it again. The first run stays on the graph, faded.

GoalRun a pass at least 40 m to one side.

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Read the graph

The horn passes 40 m to one side. Run it to the end. What pitch does the listener hear last?

Loading simulation…

Run the simulation first, then read the value off it.

When the source outruns its own sound

Try it

Set the horn's speed so it just keeps pace with the crests it sends ahead.

GoalThe horn just keeps pace with its own crests.

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Push past Mach 1 and the source reaches each new emission point before its last crest does. The circles still grow at vv about fixed centres, so they pile up along a cone trailing the source, whose half-angle satisfies

sin⁡θ=vvs=1M\sin\theta = \frac{v}{v_s} = \frac{1}{M}

where MM is the Mach number.


Try it

Set the source speed so the Mach cone has a half-angle of 45°.

GoalA Mach cone with a 45° half-angle.

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Predict

A jet cruises in a straight line at a steady Mach 1.5 for ten minutes. When does someone standing under the flight path hear the boom?

What comes next

You heard a horn hold one pitch head on and sweep beside you, and you set a source fast enough to outrun its sound. Every step of this argument used two things: a wave that travels at a speed set by its medium, and a source that keeps moving between emissions. Take away the medium and most of it survives. Light from a receding galaxy arrives stretched toward the red, and the shift is read as a speed with a closely related formula. The details differ because light needs no medium and its speed is the same for every observer, but the picture of crests laid down one at a time by something that keeps moving carries straight over.

Ideas this lesson took on

Each of these is a common intuition the lesson put to the test. If one still feels right, the section that tests it is worth another look.

  • “The siren changes its note as it goes past”
  • “The pitch climbs steadily as the source approaches”
  • “A moving source pushes its sound along faster”
  • “The sonic boom happens once, when the jet breaks the sound barrier”

Finished with this lesson?

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Research behind this lesson

  • Hrepić et al. 2010: Alongside the scientific wave model, introductory students hold an 'Entity' model in which sound is a self-standing thing distinct from the medium it travels through, plus hybrid models blending the two, which survive instruction.
  • Maurines 1992: Asked what governs how fast a signal runs along a rope or a spring, students explained the speed by the shape of the signal and the manner of its creation, how hard and how fast the flick was, rather than by the properties of the medium.
  • Wittmann et al. 1999: Students reason about a wave pulse as if it were an object, giving it the properties of a thrown ball, expecting the medium to travel with the disturbance.