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Physics

Transverse wave on a string

Physics · Waves

3D cutaway of the transverse wave on a string Open the interactive 3D model →

When you flick a rope, the bump races to the far end — so why doesn’t the rope go with it?

A wave is a moving pattern, not moving stuff. Each little piece of the rope only goes up and down, but it copies the piece next to it a moment later, so the shape travels along. The energy you put in at one end really does arrive at the other.

A transverse wave on a stretched string is a travelling disturbance in which each element moves perpendicular to the direction of propagation, while the wave pattern and its energy move along the string. Its speed is set by the medium, v = √(T/μ), and the source sets the frequency, so the wavelength follows from v = fλ.

Key facts

Wave relation
v = fλ, with k = 2π/λ and ω = 2πf
Speed on a string
v = √(T/μ)
Model rope
T = 18 N, μ = 0.5 kg/m → v = 6.0 m/s
Model range
λ = 1–4 m ↔ f = 6.0–1.5 Hz (shown 4× slower)
Power carried
P = ½ μ ω² A² v (≈ 48 W at the default λ = 2 m)
Guitar high-E string
≈ 73 N tension, v ≈ 430 m/s

Parts you can explore (12)

In the 3D model

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