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Standing waves form when waves of the same frequency and amplitude travel in opposite directions and interfere. This cheat sheet helps students connect wave diagrams, harmonic numbers, wavelengths, and resonant frequencies. It is especially useful for strings, air columns, and sound instruments.

These ideas explain why only certain frequencies produce strong vibrations in a system.

The most important relationships are between wave speed, frequency, and wavelength using v=fλv=f\lambda. For a string or open pipe, allowed wavelengths follow L=nλn2L=\frac{n\lambda_n}{2}, while a closed pipe only supports odd harmonics with L=nλn4L=\frac{n\lambda_n}{4} for odd nn. Resonance occurs when a driving frequency matches a natural frequency, causing large amplitude motion.

Nodes are points of no motion, and antinodes are points of maximum motion.

Key Facts

  • Wave speed, frequency, and wavelength are related by v=fλv=f\lambda.
  • For a string fixed at both ends, the allowed wavelengths are λn=2Ln\lambda_n=\frac{2L}{n}, where n=1,2,3,n=1,2,3,\ldots.
  • For a string fixed at both ends, the resonant frequencies are fn=nv2Lf_n=\frac{nv}{2L}.
  • For an open-open pipe, the resonant frequencies are fn=nv2Lf_n=\frac{nv}{2L}, where n=1,2,3,n=1,2,3,\ldots.
  • For a closed-open pipe, only odd harmonics occur, so fn=nv4Lf_n=\frac{nv}{4L} for n=1,3,5,n=1,3,5,\ldots.
  • Adjacent nodes or adjacent antinodes are separated by λ2\frac{\lambda}{2}.
  • A node and the nearest antinode are separated by λ4\frac{\lambda}{4}.
  • For a stretched string, wave speed is v=Tμv=\sqrt{\frac{T}{\mu}}, where TT is tension and μ\mu is linear mass density.

Vocabulary

Standing wave
A wave pattern that appears stationary because two equal waves traveling in opposite directions interfere.
Node
A point on a standing wave where the medium has zero displacement.
Antinode
A point on a standing wave where the medium has maximum displacement.
Resonance
A large amplitude vibration that occurs when a system is driven at one of its natural frequencies.
Harmonic
A resonant frequency that fits an allowed standing wave pattern in a system.
Fundamental frequency
The lowest resonant frequency of a system, usually labeled f1f_1.

Common Mistakes to Avoid

  • Using the same formula for every pipe is wrong because open-open pipes use fn=nv2Lf_n=\frac{nv}{2L}, while closed-open pipes use fn=nv4Lf_n=\frac{nv}{4L} for odd nn only.
  • Counting harmonics incorrectly in a closed-open pipe is wrong because closed-open pipes have n=1,3,5,n=1,3,5,\ldots and do not include even harmonics.
  • Confusing nodes and antinodes is wrong because a node has zero displacement, while an antinode has maximum displacement.
  • Forgetting that v=fλv=f\lambda must use consistent units is wrong because length must usually be in meters, frequency in hertz, and speed in meters per second.
  • Assuming resonance always means infinite amplitude is wrong because real systems lose energy through damping, friction, and sound radiation.

Practice Questions

  1. 1 A string fixed at both ends has length L=0.80mL=0.80\,\text{m} and wave speed v=120m/sv=120\,\text{m/s}. What is the fundamental frequency f1f_1?
  2. 2 An open-open pipe has length L=0.50mL=0.50\,\text{m} and sound speed v=343m/sv=343\,\text{m/s}. Find the first three resonant frequencies.
  3. 3 A closed-open pipe has length L=0.25mL=0.25\,\text{m} and sound speed v=340m/sv=340\,\text{m/s}. What are the first and third allowed harmonic frequencies?
  4. 4 Explain why a closed-open pipe has only odd harmonics, using the locations of nodes and antinodes at the pipe ends.