Mechanical Waves & Sound

AP Physics 1 study guide for mechanical waves and sound: wave properties, standing waves, interference, resonance, and the Doppler effect.

# Mechanical Waves & Sound — AP Physics 1

Waves transfer energy without transferring matter. AP Physics 1 covers the properties of mechanical waves (including sound), superposition, standing waves, and resonance. Understanding wave behavior is important for both the multiple-choice and free-response sections.

Key Concepts

Wave Properties

  • Wavelength (λ\lambda): distance between successive crests (or any two equivalent points).
  • Frequency (ff): number of complete cycles per second (Hz).
  • Period (T=1/fT = 1/f): time for one complete cycle.
  • Amplitude (AA): maximum displacement from equilibrium.
  • Wave speed: v=fλv = f\lambda

Transverse vs. Longitudinal Waves

  • Transverse: oscillation is perpendicular to wave travel (e.g., waves on a string).
  • Longitudinal: oscillation is parallel to wave travel (e.g., sound waves).

Wave Speed on a String

v=FTμv = \sqrt{\frac{F_T}{\mu}} where FTF_T is tension and μ=m/L\mu = m/L is linear mass density.

Superposition and Interference

  • Constructive interference: waves add (crest + crest).
  • Destructive interference: waves cancel (crest + trough).
  • The resultant displacement is the sum of individual displacements.

Standing Waves

Formed by superposition of two waves traveling in opposite directions.

On a string fixed at both ends:

  • Wavelengths: λn=2Ln\lambda_n = \frac{2L}{n} for n=1,2,3,n = 1, 2, 3, \ldots
  • Frequencies: fn=nv2Lf_n = \frac{nv}{2L}
  • n=1n = 1: fundamental (first harmonic)

In an open pipe (open at both ends):

  • Same as string: fn=nv2Lf_n = \frac{nv}{2L}, all harmonics.

In a closed pipe (closed at one end):

  • fn=nv4Lf_n = \frac{nv}{4L}, odd harmonics only (n=1,3,5,n = 1, 3, 5, \ldots).

Sound

  • Sound is a longitudinal mechanical wave.
  • Speed of sound in air: 343 m/s\approx 343\ \text{m/s} at 20°C20°\text{C}.
  • Intensity relates to amplitude squared; loudness is measured in decibels.

Doppler Effect (Conceptual)

  • Source moving toward observer: frequency increases (higher pitch).
  • Source moving away: frequency decreases (lower pitch).

Worked Example

Problem: A guitar string of length 0.65 m0.65\ \text{m} has a fundamental frequency of 330 Hz330\ \text{Hz}. What is the wave speed on the string?

Solution:

Fundamental: f1=v/(2L)f_1 = v/(2L)

v=2Lf1=2(0.65)(330)=429 m/sv = 2Lf_1 = 2(0.65)(330) = 429\ \text{m/s}

Practice Questions

  1. 1. A wave has frequency 500 Hz500\ \text{Hz} and wavelength 0.68 m0.68\ \text{m}. What is the wave speed?

    v=fλ=500×0.68=340 m/sv = f\lambda = 500 \times 0.68 = 340\ \text{m/s}.

    2. A string vibrates in its third harmonic with L=1.2 mL = 1.2\ \text{m}. What is the wavelength?

    λ3=2L/3=2(1.2)/3=0.8 m\lambda_3 = 2L/3 = 2(1.2)/3 = 0.8\ \text{m}.

    3. A closed pipe is 0.5 m0.5\ \text{m} long. What is the fundamental frequency? (Use v=340 m/sv = 340\ \text{m/s}.)

    f1=v/(4L)=340/(4×0.5)=170 Hzf_1 = v/(4L) = 340/(4 \times 0.5) = 170\ \text{Hz}.

    4. Two speakers emit the same frequency in phase. At a point equidistant from both, is the interference constructive or destructive?

    Constructive — the path difference is zero, so the waves arrive in phase.

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Summary

  • Wave speed: v=fλv = f\lambda.
  • Standing waves form at specific resonance frequencies determined by boundary conditions.
  • Open pipes support all harmonics; closed pipes support only odd harmonics.
  • Sound is a longitudinal wave; the Doppler effect shifts frequency based on relative motion.

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