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Waves & Sound · Physics

Energy of a Travelling Wave: 3D Simulation

A sine wave runs along a 3D string, each bead glowing by its energy. The surprise: kinetic and stretch energy both peak where the string crosses its rest line, not at the crests. Change amplitude, frequency, speed and mass per metre and watch the power P = ½μω²A²v.

Interactive virtual lab · no download · works on phones and laptops

Chapter
Waves
For
Class 11 · JEE
Time
~15 min

Energy of a Travelling Wave is a Pro simulation

Pro opens all 152 virtual labs — 693 simulations with guides and quizzes.

How to use it

  1. 1Pick a module from the list (2); set your level at the top right for more controls.
  2. 2Change amplitude, frequency, speed and mass per metre; the wave runs by itself.
  3. 3Use Predict before you look, then Derive, Questions, Practise and Compare.

What to notice

  • Kinetic and potential energy per metre are equal at every point: ½μω²A²cos²(kx − ωt).
  • Both peak at the zero crossings, where the string moves fastest and is stretched most.
  • A crest is momentarily at rest and flat: no energy there.
  • Power ∝ A² and ∝ ω²: double either and see what happens.

For teachers

A ready-made teaching kit comes with this lab

  • Lesson plan

    21 min, 4 steps

  • Ask the class

    3 questions with answers

  • Quick quiz

    5 questions, printable

  • Key formulas

    3 formulas

About the Energy of a Travelling Wave simulation

A wave on a string carries energy, but where on the wave is it? This 3D energy of a travelling wave simulation makes each bead glow by the energy it holds and draws the kinetic and stretch energy per metre underneath as the wave runs. The answer surprises most students: both kinds of energy peak where the string crosses its rest line, where it moves fastest and slopes most steeply, while at a crest a bead is momentarily still and the string there is flat — no energy at all.

This is the difference between a travelling wave and a single mass on a spring, where kinetic and potential energy swap. On the string they are equal at every point, both ½μω²A²cos²(kx − ωt), because the tension T = μv² makes Tk² equal μω². The second module turns that into the power a wave delivers, P = ½μω²A²v: double the amplitude or the frequency and the power goes up four times. Change amplitude, frequency, speed and mass per metre, predict, derive and practise numericals at JEE level.

Also covers: energy of a wave, energy carried by a wave on a string, power of a wave, intensity of wave, kinetic energy density, potential energy density, ½μω²a²v, power proportional to amplitude squared, strain in a wave, class 11 waves, jee waves energy.

Frequently asked questions

Where is the energy of a travelling wave on a string?

At the points where the string crosses its equilibrium line. There each element moves fastest (most kinetic energy) and the string is steepest, so most stretched (most potential energy). At the crests and troughs both are zero.

What is the power transmitted by a wave on a string?

P = ½μω²A²v, where μ is mass per metre, ω the angular frequency, A the amplitude and v the wave speed. It is the average energy per metre, ½μω²A², carried along at speed v.

How does the power of a wave depend on amplitude and frequency?

It goes as the square of each: doubling the amplitude or doubling the frequency each makes the power four times larger. This is why intensity of sound and light also goes as amplitude squared.