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Waves & Sound

Wave Pulses & Superposition

A shape crosses the whole rope while the rope itself stays home, and two pulses pass straight through each other without a scratch.

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Wave Pulses & Superposition

A shape crosses the whole rope while the rope itself stays home, and two pulses pass straight through each other without a scratch.

35 min4 checkpoints9 simulation tasks

Introduction

Flick a taut rope once and a hump runs to the far end, while the rope itself stays where it was.

Predict

You flick the rope twice as hard, so the pulse is twice as tall. How long does it now take to reach the far end?

What sets the speed

Try it

This pulse is 0.30 m tall. Make it twice as tall, run it, and read when it reaches the far end.

GoalRun a pulse 0.60 m tall.

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Try it

Now change the rope instead. Set the tension so the pulse reaches the far end in half the time, 0.375 s.

GoalReach the far end at 0.375 s.

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Tension and mass per metre

The speed of a pulse on a stretched string depends on two properties of the rope, its tension TT and its mass per metre μ\mu, and nothing else:

v=Tμ\vel{v} = \sqrt{\frac{T}{\mu}}

Every mechanical wave follows this pattern: a restoring influence on top, an inertia underneath, the square root of the ratio.


Try it

This rope is twice as heavy per metre, so the pulse now arrives late. Set the tension so it reaches the far end at 0.750 s again.

GoalReach the far end at 0.750 s again.

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Try it

The far end is 4.5 m away. Choose any tension and any rope that make the pulse take 1.00 s to get there.

GoalReach the far end at 1.00 s.

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The medium stays home

The pulse crosses the whole rope. Watch the beads threaded along it: they sit at fixed values of xx, and only their heights change.

Predict

A single element of the rope is marked at x = 3 m, on its own dashed vertical rail. What does it do as the pulse passes?

Predict

The pulse starts at x=1.5x = 1.5 m and moves right at 6 m/s. Sketch the height of the marked element at x=3x = 3 m for the first half second.

Loading the graph

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What the end does to the pulse

Try it

The far end is clamped. Run the pulse there and back, and watch the marked element as the pulse passes it each way.

GoalWatch which way up the pulse comes home.

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Predict

The far end is a ring free to slide up and down a frictionless post. An upright pulse arrives. What travels back?

Try it

The marked element sits half a metre from the far end. Change the ends so the pulse comes home the right way up, and run it.

GoalSend the pulse home the right way up.

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Two pulses at once

Now a second pulse starts from x=4.5x = 4.5 m at the same instant, upside down, heading the other way. At t=0.25t = 0.25 s the two meet in the middle, and the string is flat from end to end.

Predict

At t = 0.25 s the string is flat from end to end. What happens in the next instant?

Try it

The marked element sits in the middle of the string. Choose a second pulse that keeps it perfectly still while pulses run through it.

GoalKeep the middle of the string still for the whole run.

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Try it

Now make the middle of the string rise to twice the height of either pulse.

GoalLift the middle of the string to twice the pulse height.

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What comes next

You changed what sets a pulse's speed, flipped it at a clamp, and made two pulses cancel and add. Send pulses continuously instead, and the reflections start arriving back on top of the pulses still going out. Usually the result is a mess, but at certain frequencies it organises itself into a pattern that does not travel at all. That is the next lesson.

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.

  • “A bigger pulse travels faster”
  • “The rope travels along with the pulse”
  • “A reflection always comes back flipped”
  • “Two pulses that cancel have destroyed each other”

Finished with this lesson?

Progress is stored on this device only. There is no account and nothing is sent anywhere.

Research behind this lesson

  • 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.
  • Tongchai et al. 2009: The Mechanical Waves Conceptual Survey: 22 multiple-choice items covering propagation, superposition, reflection and standing waves, whose distractors were built from students' own open-ended answers and follow-up interviews rather than invented to look plausible.
  • 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.
  • Wittmann 2002: Interview and written-response analysis showing students use both event-like and object-like descriptions of wave pulses but reason predominantly from object properties: treating a pulse as a thing with a size and a weight rather than as a disturbance passing through a medium.