3.4 Sound
Objective
Explain how changes in amplitude and frequency affect the loudness and pitch of sound waves, and understand the related concepts required by the Cambridge IGCSE/A‑Level Physics syllabus.
1. Production of Sound
- A sound is produced when a source vibrates, causing the particles of a surrounding medium to oscillate about their equilibrium positions.
- The oscillating particles generate alternating regions of:
- Compression – a region of higher pressure (particles pushed together).
- Rarefaction – a region of lower pressure (particles spread apart).
- These compressions and rarefactions travel through the medium as a longitudinal wave.
2. Nature of Sound Waves
- Longitudinal wave: particle displacement is parallel to the direction of wave propagation.
- In solids a transverse (shear) component can also exist, but ordinary sound in gases and liquids is purely longitudinal.
Key Terms
| Term | Symbol | Definition |
|---|
| Amplitude | A | Maximum displacement of particles from their rest position. |
| Frequency | f | Number of complete vibrations per second (Hz). |
| Wavelength | λ | Distance between successive compressions (or rarefactions). |
| Speed of sound | v | Rate at which the disturbance travels through the medium. |
| Period | T | Time for one complete vibration (T = 1/f). |
3. Speed of Sound
The speed of sound depends on the medium’s elasticity and density. In general:
- Sound travels fastest in solids, slower in liquids, and slowest in gases.
- Typical values (20 °C):
- Air: v ≈ 340 m s⁻¹ (range 330–350 m s⁻¹)
- Water: v ≈ 1500 m s⁻¹
- Steel: v ≈ 5000 m s⁻¹
The fundamental relationship is
\(v = f\lambda\)
Practical Determination of the Speed of Sound (AO3)
- Place a loudspeaker and a microphone a known distance \(d\) apart (e.g., 5 m).
- Emit a short pulse (or a burst of a known frequency) from the speaker.
- Measure the time‑of‑flight \(t\) between emission and detection using an oscilloscope or digital timer.
- Calculate the speed: \(\displaystyle v = \frac{d}{t}\).
- Repeat at least three times, record the spread of results and estimate the uncertainty (AO2).
4. Amplitude, Intensity and Loudness
- The intensity \(I\) (power per unit area) of a sound wave is proportional to the square of its amplitude:
\(I \propto A^{2}\)
A more complete expression for a plane progressive wave in a fluid is
\(I = \frac{1}{2}\,\rho v \omega^{2} A^{2}\)
where \(\rho\) is the density of the medium and \(\omega = 2\pi f\) the angular frequency.
- Loudness is a logarithmic response to intensity. The sound‑level \(L\) in decibels (dB) is defined as
\(L = 10\log{10}\!\left(\dfrac{I}{I{0}}\right)\)
with \(I_{0}=1\times10^{-12}\,\text{W m}^{-2}\) (threshold of hearing).
- Consequences:
- Doubling the amplitude → intensity increases by a factor of four → sound level rises by \(10\log_{10}4 \approx 6\) dB (perceptibly louder).
- Halving the amplitude → intensity falls to one‑quarter → level drops by ≈ 6 dB (softer).
5. Frequency and Pitch
6. Echo, Reverberation and Ultrasound
7. Combined Effects of Amplitude and Frequency
- Amplitude controls loudness; frequency controls pitch. They are independent, but many real sounds vary both simultaneously.
- Examples:
- Piano – Striking a key harder increases the amplitude (louder) and, because the hammer strikes the string slightly closer to its centre, may raise the frequency a few cents (sharper pitch).
- Loudspeaker volume control – Adjusts the amplitude of the electrical signal; pitch remains unchanged.
- Human voice – Speaking loudly requires larger air‑pressure variations (greater amplitude). Changing the tension or length of the vocal cords changes frequency (pitch).
8. Practical Examples (Application of Concepts)
- String instrument (e.g., guitar) – Tightening a string increases tension, raising the frequency (higher pitch). Plucking harder increases amplitude (louder note).
- Loudspeaker – The volume knob varies the amplitude of the audio signal; the pitch of the music is unchanged.
- Human voice – Loud speech → larger amplitude of air‑pressure variations. Pitch changes are produced by altering the length/tension of the vocal cords.
- Ultrasound scanner – Generates high‑frequency pulses (≈2–15 MHz). Reflected echoes are processed to form an image of internal body structures.
9. Common Misconceptions
- Loudness ≠ Pitch – Loudness depends on amplitude/intensity; pitch depends on frequency.
- High pitch does not guarantee loudness – A high‑frequency tone can be very soft if its amplitude is low.
- Sound travels faster in denser media – It travels fastest in media that are both dense and highly elastic (e.g., steel ≫ water ≫ air).
- Amplitude and frequency are unrelated – While mathematically independent, many real sources (e.g., musical instruments) change both when the player varies effort.
10. Summary Table
| Parameter | Increase | Decrease | Perceptual Effect |
|---|
| Amplitude (A) |
| Amplitude | Higher | Lower | Louder (higher dB) / softer |
| Frequency (f) |
| Frequency | Higher | Lower | Higher pitch (treble) / lower pitch (bass) |
| Speed of Sound (v) |
| Medium | More elastic & denser (e.g., steel) | Less elastic (e.g., air) | Faster propagation / slower propagation |
11. Suggested Diagrams (for classroom use)
- Longitudinal wave diagram showing compressions, rarefactions, amplitude (vertical displacement of particles), wavelength, and direction of propagation.
- Time‑of‑flight set‑up for measuring the speed of sound, with labelled speaker, microphone, distance \(d\) and oscilloscope trace.
- Echo illustration: source → reflecting surface → listener, with the round‑trip distance indicated.
- Ultrasound transducer emitting high‑frequency pulses into a tissue phantom and receiving echoes.
- Graph of sound‑level (dB) versus amplitude, highlighting the 6 dB change for a doubling of amplitude.
Key Take‑away
In sound waves, amplitude determines loudness through intensity and the decibel scale, while frequency determines pitch. The speed of sound varies with the medium (solids > liquids > gases) and is linked to frequency and wavelength by \(v = f\lambda\). Understanding these relationships enables students to analyse musical tones, solve acoustic‑engineering problems, and appreciate applications such as medical ultrasound and echo ranging.