Sound is a mechanical wave that travels through a medium (usually air) by the vibration of particles. When a source vibrates, it pushes and pulls on the surrounding air molecules, creating a series of compressions and rarefactions that propagate as a wave.
Think of a rubber band being stretched and released – the band’s motion pushes on the air around it, just like a vibrating string does.
| Source | Example | Frequency Range (Hz) | Typical Amplitude |
|---|---|---|---|
| String | Guitar string | 80–1000 | Small |
| Air column | Flute | 200–2000 | Medium |
| Vibrating membrane | Drum head | 50–500 | Large |
| Speaker cone | Loudspeaker | 20–20 000 | Variable |
| Human voice | Singing | 85–255 | Small–Medium |
The fundamental relationships that describe sound waves are:
Tip 1: When asked to calculate frequency, always check if the problem involves a string, air column or a vibrating membrane and use the appropriate formula.
Tip 2: Remember that amplitude is proportional to the displacement of the source. If a source vibrates with a larger amplitude, the resulting sound will be louder.
Tip 3: Use the temperature correction for the speed of sound: \$v = 331 + 0.6T\$. This is handy for problems involving different temperatures.
Tip 4: When comparing loudness, use the decibel formula \$L = 20\log{10}\frac{P}{P0}\$. A 10 dB increase means the intensity is ten times greater.
Tip 5: For questions about wave propagation, remember that sound travels as a longitudinal wave – the particles move parallel to the direction of travel.
• Sound is a pressure wave created by vibrating sources.
• The speed of sound depends on temperature: \$v = 331 + 0.6T\$.
• Frequency of a vibrating string: \$f = \frac{1}{2L}\sqrt{\frac{T}{\mu}}\$.
• Sound intensity increases with the square of amplitude.
• Loudness is measured in decibels: \$L = 20\log{10}\frac{P}{P0}\$.
• Different sources (strings, membranes, air columns) produce different frequency ranges.