Lesson 12: Waves & Sound

Week 12 โ€” Vibrations, waves, and the physics of sound

๐ŸŽฏ Learning Objectives

๐ŸŽฏ Intuition First: What Is a Wave?

Think of a stadium "wave" โ€” people stand up and sit down, but they don't move from their seats. The disturbance travels around the stadium, but the people don't. That's a wave: a disturbance that transfers energy without transferring matter.

๐Ÿ’ก Two Types:
  • Transverse waves: disturbance perpendicular to direction of travel (light, waves on a string)
  • Longitudinal waves: disturbance parallel to direction of travel (sound, compression waves)

๐Ÿ“‹ Wave Properties

Wave speed: v = fฮป   (frequency ร— wavelength)
Frequency: f (Hz = cycles per second)
Angular frequency: ฯ‰ = 2ฯ€f
Wave number: k = 2ฯ€/ฮป

๐Ÿ“‹ Wave Equation

y(x,t) = A sin(kx โˆ’ ฯ‰t) (traveling wave)

๐Ÿ“‹ Superposition and Interference

When two waves overlap, their displacements add:

ytotal = yโ‚ + yโ‚‚

๐Ÿ“‹ Standing Waves

When two identical waves traveling in opposite directions overlap, they create a standing wave with nodes (no motion) and antinodes (max motion):

Fixed string: ฮปโ‚™ = 2L/n,   fโ‚™ = nv/2L   (n = 1, 2, 3, ...)

n = 1 is the fundamental (first harmonic), n = 2 is the second harmonic (first overtone), etc.

๐Ÿ“ Worked Example: Guitar String

A guitar string (length 0.65 m, mass 3 g) is stretched under tension of 80 N. What is the fundamental frequency?

Step 1 โ€” Linear mass density:

ฮผ = m/L = 0.003/0.65 = 0.00462 kg/m

Step 2 โ€” Wave speed on string:

v = โˆš(T/ฮผ) = โˆš(80/0.00462) = โˆš17,316 = 131.6 m/s

Step 3 โ€” Fundamental frequency:

fโ‚ = v/2L = 131.6/(2 ร— 0.65) = 131.6/1.30 = 101 Hz

โœ… Fundamental โ‰ˆ 101 Hz (roughly the note C)

๐Ÿ“‹ The Doppler Effect

When source and observer move relative to each other, the observed frequency shifts:

fobs = fs ร— (v ยฑ vobs) / (v โˆ“ vs)

Sign convention:

๐Ÿ’ก Everyday Example:

An ambulance siren sounds higher-pitched as it approaches and lower-pitched as it moves away. The frequency doesn't change โ€” your ear perceives it differently due to relative motion.

๐Ÿ“ Worked Example: Doppler Effect

A car horn (f = 500 Hz) is mounted on a car moving toward you at 30 m/s. What frequency do you hear? (vsound = 343 m/s)

fobs = fs ร— v / (v โˆ’ vs) = 500 ร— 343 / (343 โˆ’ 30)
fobs = 500 ร— 343/313 = 500 ร— 1.096 = 548 Hz

โœ… You hear 548 Hz (higher than the actual 500 Hz)

๐Ÿ“‹ Sound Intensity and Decibels

Intensity: I = P/A (power per unit area, W/mยฒ)
Decibel level: ฮฒ = 10 logโ‚โ‚€(I/Iโ‚€)

where Iโ‚€ = 10โปยนยฒ W/mยฒ (threshold of hearing).

โœ๏ธ Practice Problems

Problem 1: A wave has frequency 200 Hz and wavelength 1.5 m. What is its speed?

Problem 2: A source (f = 1000 Hz) moves toward you at 50 m/s. What frequency do you hear? (v = 340 m/s)

Problem 3: A 2-m string has its 3rd harmonic at 300 Hz. What is the fundamental frequency?

โœ… Check Your Understanding

Q1: Can two waves cancel each other completely? When?

Click to reveal answer

Yes! When two identical waves are exactly out of phase (180ยฐ or ฯ€ radians apart), their displacements are equal and opposite at every point: A + (โˆ’A) = 0. This is perfect destructive interference. Noise-canceling headphones use this principle!

Q2 (mini-problem): What is the decibel level of a sound with intensity 10โปโถ W/mยฒ? (Iโ‚€ = 10โปยนยฒ W/mยฒ)

Click to reveal answer
ฮฒ = 10 logโ‚โ‚€(10โปโถ/10โปยนยฒ) = 10 logโ‚โ‚€(10โถ) = 10 ร— 6 = 60 dB

Answer: 60 dB (about the level of normal conversation)