Theory & learning

Every idea as a card: definition, key points, formulas, examples and the mistakes to avoid.

Introduction to sound

Sound is energy from vibration

Sound is a form of energy that produces the sensation of hearing. It is always produced by a vibrating object — a rapid to-and-fro motion.

  • Sound needs a material medium (solid, liquid or gas), so sound waves are mechanical waves.
  • A vibrating object moving forward compresses the air in front of it, creating a compression.
  • Moving backwards it leaves a region of low pressure, a rarefaction.
  • A repeating series of compressions and rarefactions travels outward as a longitudinal wave.
Remember

No medium, no sound. Light can cross vacuum; sound cannot.

Did you know? A bell ringing inside a vacuum jar can be seen vibrating but not heard at all.

Terms of a sound wave

Wavelength, frequency, period, amplitude, speed

Five quantities describe every sound wave. Learn them together — they are linked by one equation.

  • Wavelength (λ): distance between two consecutive compressions or two consecutive rarefactions. Unit: metre.
  • Frequency (f): number of complete vibrations per second. Unit: hertz. It is fixed by the source and does not change when the wave enters another medium.
  • Time period (T): time for one complete wave to pass a point. Unit: second.
  • Amplitude (A): maximum displacement of a medium particle from its mean position. Unit: metre.
  • Speed (v): distance travelled by the wave per second. Unit: m/s. In the same conditions it is the same for all frequencies.
v = f λ

Wave equation linking speed, frequency and wavelength.

T = 1 / f

Time period is the reciprocal of frequency.

Common mistake

Frequency does not change when sound moves from air into water — the speed and wavelength change instead.

Natural vibrations

Free vibration with constant amplitude

The periodic vibrations of a body in the absence of any external force are called natural or free vibrations. The frequency with which it vibrates is its natural frequency and the corresponding period is its natural period — both are decided only by the body itself.

  • Amplitude and frequency both stay constant, so the total energy of the body is conserved and no energy is lost.
  • These vibrations are simple harmonic: the only force acting is the restoring force, which is proportional to the displacement and directed towards the mean position.
  • Truly constant-amplitude vibration is only possible in vacuum; any medium offers resistance, so in practice free vibrations always die out.
  • Natural frequency depends on the size, shape, mass, tension and material (elasticity) of the body — not on how hard you disturb it.
  • Striking the body harder increases the amplitude and the loudness, but the frequency (pitch) stays exactly the same.
  • For a simple pendulum the period depends only on length and gravity, and is independent of the mass of the bob and of the amplitude (for small swings).
  • A stretched string can vibrate in several modes (fundamental and overtones); the lowest frequency mode is the fundamental note.
ω = √(k / m)

Angular natural frequency of a loaded spring.

T = 2π √(m / k)

Natural period of a loaded spring.

T = 2π √(l / g)

Natural period of a simple pendulum of length l.

f = 1 / T

Natural frequency in hertz — vibrations completed each second.

f = (1 / 2l) √(T / m)

Fundamental frequency of a stretched string of length l, tension T and mass per unit length m.

Common mistake

Natural frequency does not depend on the amplitude. Hitting a tuning fork harder makes a louder note, never a higher-pitched one.

Remember

In a stretched string the modes have frequencies in the ratio 1 : 2 : 3 and wavelengths in the ratio 6 : 3 : 2.

Did you know? A pendulum clock runs slow when taken up a mountain: g is smaller there, so T = 2π√(l/g) becomes longer.

Damped vibrations

Amplitude that dies away

The periodic vibrations of a body of decreasing amplitude in the presence of a resistive force are called damped vibrations.

  • Two forces act: the restoring force and the frictional or resistive force of the medium.
  • Each vibration loses some energy as heat, so the amplitude falls steadily.
  • How fast it dies depends on the viscosity and density of the medium and on the shape and size of the body.
  • The frequency of damped vibration is slightly less than the natural frequency.
x = A e^(−bt/2m) cos(ω t)

Cosine gives the rhythm; the exponential envelope shrinks the amplitude.

Remember

Every real natural vibration in a medium is in fact a damped vibration.

Forced vibrations

Vibration under an external periodic force

Vibrations of a body under the influence of an external periodic force are called forced vibrations. Three forces act: restoring, resistive and the external driving force.

  • The body gradually gives up its own natural frequency and vibrates at the frequency of the applied force.
  • The amplitude depends on how close the driving frequency is to the natural frequency, and it does not change with time.
  • If the two frequencies are far apart the amplitude is very small.
  • The energy lost to damping is continuously replaced by the external force.

Common mistake

Forced vibration is not the same as resonance. Resonance is the special case when the two frequencies are exactly equal.

Resonance

A special case of forced vibration

When the frequency of the external periodic force equals the natural frequency of the body, the body vibrates with a greatly increased amplitude. This is resonance, and the large vibrations are resonant vibrations.

  • Conditions: the applied frequency must exactly equal the natural frequency, and the force must actually produce forced vibration in the body.
  • The amplitude at resonance is limited by the frictional forces present — less damping gives a taller, sharper peak.
  • At resonance the body vibrates in phase with the driver and radiates a large amount of energy, so a loud sound is heard.
  • Resonant vibrations continue for a long time after the external force stops; ordinary forced vibrations die at once.
A = (F₀/m) / √((ω₀² − ω²)² + (2γω)²)

Amplitude of a driven oscillator; maximum when ω = ω₀.

Remember

Soldiers break step on a suspension bridge to avoid driving it at its natural frequency.

Did you know? The Tacoma Narrows Bridge collapse of 1940 is the most famous resonance disaster.

Comparison table

Natural vs damped vs forced

The examiner's favourite table. Compare frequency, amplitude and energy across the three.

FeatureNaturalDampedForced
DefinitionPeriodic vibrations with no external force actingPeriodic vibrations of decreasing amplitude in a resistive mediumVibrations under an external periodic force
FrequencyDepends on the size and shape of the body; stays constantSlightly less than the natural frequency; decrease depends on dampingEqual to the frequency of the applied force
AmplitudeConstant with timeFalls steadily and the vibrations finally stopDepends on the applied frequency; constant with time
EnergyNo loss of energySome energy lost as heat in each vibrationLoss made up by the external force
ExamplePendulum swinging in vacuumPendulum swinging in air or waterTuning fork stem pressed on a table top
Echo

Sound that comes back

The repetition of sound caused by the reflection of sound waves is called an echo. Because a sound sensation persists in the brain for about 0.1 s, the reflected sound must arrive at least 0.1 s later to be heard separately.

  • In air at 344 m/s, sound covers 34.4 m in 0.1 s, so the reflector must be at least 17.2 m away.
  • Closer than about 17 m, the reflected sound merges with the original.
  • Repeated reflections that prolong sound in a hall are called reverberation; rolling thunder is a natural example.
  • In sea water (v ≈ 1400 m/s) the minimum distance becomes about 70 m.
  • The reflector must be large compared with the wavelength, and the original sound loud and short.
d = v t / 2

Distance to the reflector, since the sound travels there and back.

Did you know? Bats fly far slower than sound, which is why their echoes reach them in time to steer.

Characteristics of sound

Loudness, pitch and quality

Two sounds are distinguished by loudness, pitch (shrillness) and quality (timbre). Each has a subjective sensation and an objective, measurable partner.

  • Loudness is the sound energy reaching the ear per second; it depends on amplitude, and is a sensation. Its objective partner is intensity, measured in W/m². Loudness is measured in phons, sound level in decibel.
  • Loudness ∝ (amplitude)², falls as 1/(distance)², and grows with the vibrating surface area, the density of the medium and the presence of a resonating body.
  • Pitch depends on frequency: higher frequency gives a shriller note. Pitch is subjective; frequency is objective.
  • Quality depends on the wave form. Two sounds of the same amplitude and frequency from different instruments differ in wave shape.
  • A musical sound has a regular, periodic wave form; noise has an irregular wave form with sudden changes in amplitude.
Common mistake

Loudness and intensity are not the same. Intensity is measurable; loudness also depends on the listener's ear.