Describe the production of sound by vibrating sources
3.4 Sound – Production of Sound by Vibrating Sources 🎵
What is Sound?
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.
How Vibrating Sources Produce Sound
- The source (e.g. a guitar string, a speaker cone or a drum head) starts to vibrate.
- The vibration displaces nearby air molecules, creating alternating regions of high and low pressure.
- These pressure variations travel through the air as a longitudinal wave until they reach our ears.
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.
Types of Vibrating Sources
| 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 |
Key Equations
The fundamental relationships that describe sound waves are:
- Speed of sound in air: $$v = 331 + 0.6T$$ where $T$ is temperature in °C.
- Frequency of a vibrating string: $$f = \frac{1}{2L}\sqrt{\frac{T}{\mu}}$$ where $L$ is length, $T$ is tension, and $\mu$ is mass per unit length.
- Frequency of a standing wave in an air column: $$f = \frac{nv}{2L}$$ where $n$ is the harmonic number.
- Amplitude of a simple harmonic oscillator: $$A = \frac{F}{m\omega^2}$$ where $F$ is driving force, $m$ mass, and $\omega$ angular frequency.
- Pressure amplitude of a sound wave: $$\Delta P = \rho v \omega A$$ where $\rho$ is air density.
- Sound intensity: $$I = \frac{1}{2}\rho v \omega^2 A^2$$.
- Decibel level: $$L = 20\log_{10}\frac{P}{P_0}$$ where $P$ is sound pressure and $P_0 = 2\times10^{-5}\,\text{Pa}$.
Exam Tips
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 $L = 20\log_{10}\frac{P}{P_0}$. 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.
Key Concepts Summary
• 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: $L = 20\log_{10}\frac{P}{P_0}$.
• Different sources (strings, membranes, air columns) produce different frequency ranges.
Revision
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