Section 8.6: Standing Waves

A standing wave is formed when two waves of the same frequency and amplitude travel in opposite directions and interfere. Unlike traveling waves, the energy does not propagate; nodes remain stationary while antinodes oscillate maximally.

General form: \[ y(x,t) = 2A \sin(kx) \cos(\omega t) \]

Where:
\( A \) = amplitude of individual waves
\( k \) = wave number \( (2\pi/\lambda) \)
\( \omega \) = angular frequency \( (2\pi f) \)

Nodes: points of zero displacement \( (\sin(kx)=0) \)
Antinodes: points of maximum displacement \( (\sin(kx)=\pm 1) \)

Example: String Fixed at Both Ends

A string of length 1 m is fixed at both ends. If the string vibrates in its 2nd harmonic (n=2) with speed of wave 200 m/s, find its frequency.

Wavelength of 2nd harmonic: \( \lambda = \frac{2L}{n} = \frac{2 \cdot 1}{2} = 1 \text{ m} \)
Frequency: \( f = \frac{v}{\lambda} = \frac{200}{1} = 200 \text{ Hz} \)

Practice Problems

  1. A string 0.8 m long fixed at both ends vibrates in the 3rd harmonic. Wave speed is 160 m/s. Find the frequency.
  2. A pipe closed at one end has a length of 0.85 m. Find the wavelength of the fundamental mode.
  3. Explain why nodes in standing waves do not move while antinodes oscillate.
  4. Two waves traveling in opposite directions produce a standing wave with amplitude 5 cm. What is the maximum displacement at an antinode?
  5. Derive the condition for standing waves in a string fixed at both ends.