Explain why a stretched string fixed at both ends can only vibrate at certain discrete frequencies.

IB DP Physics Standard Level (2023 syllabus) — C.4 Standing waves and resonance · Explain · 4 marks · View as Markdown

Written & reviewed by James Millett — Biology (Imperial College London), PGCE Science (University of Cambridge).

A musician plucks a stretched string that is fixed at both ends. The string is observed to vibrate in several different patterns, each at a specific frequency.

Model answer (4 marks)

A standing wave is produced by the superposition of two waves travelling in opposite directions along the string.

Because the string is fixed at both ends, the ends must be nodes – points of zero displacement. Therefore only whole numbers of half‑wavelengths can fit between the two fixed ends.

This boundary condition limits the allowed wavelengths to a discrete set: λ = 2L/n, where n = 1, 2, 3… is the mode number.

The wave speed on the string is fixed for a given tension and mass per unit length, so each allowed wavelength corresponds to a unique frequency f = v/λ. Hence the string can vibrate only at a discrete set of resonant frequencies.

Examiner tips

  • Show the standing‑wave picture and explain the node condition; use the formula λ = 2L/n; link λ to f via f = v/λ; keep the answer concise and use the exact terminology.
  • Use the word "discrete" and emphasise the boundary condition at the fixed ends.

Mark scheme (4 marks)

  1. A standing wave is formed by the superposition (interference) of two waves travelling in opposite directions along the string.
  2. The fixed ends of the string must be nodes (zero displacement), so only whole numbers of half-wavelengths fit between the two fixed ends.
  3. This boundary condition restricts the allowed wavelengths to a discrete set (λ = 2L/n), so only specific wavelengths can form stable standing waves.
  4. Since wave speed on the string is fixed (for given tension and mass per unit length), each allowed wavelength corresponds to a unique frequency (f = v/λ), giving a discrete set of resonant frequencies.

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