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The Limits of Hearing

13 min read4 ideas6 checks2 figures to playBy Asheshanand Acharya
What you will learn 0 / 4
The audible range of frequencies
Maths you need
Look around
A whistle only the dog hears

A trainer at a dog show lifts a small silver whistle and blows hard. You hear nothing at all. Yet the dog across the ground turns at once and runs to her. The whistle made a sound, and it was loud enough for the dog. It was simply not a sound that a human ear can hear.

you will find the limits of human hearing in frequency and in intensity, and what makes two instruments sound different on the same note.

The range of frequencies

Human hearing is limited both in frequency and in intensity. For most healthy young listeners, the audible frequency range extends from approximately \(20\,\text{Hz}\) to \(20\,\text{kHz}\). This is the audible range. Frequencies below \(20\,\text{Hz}\) are called infrasound, whereas frequencies above \(20\,\text{kHz}\) are called ultrasound.

The range of frequencies we hearA horizontal frequency axis on a logarithmic scale from 10 hertz to 100 000 hertz, with ticks at 10, 100, 1000, 10 000 and 100 000. Three shaded bands lie on it: infrasound below 20 hertz, the audible range from 20 to 20 000 hertz, and ultrasound above 20 000 hertz. A slider sets the frequency f as a power of ten, from 20 hertz to 20 kilohertz; a dot marks it on the axis, and a readout gives f and the wavelength of that sound in air, 340 metres per second divided by f: 17 metres at 20 hertz and 1.7 centimetres at 20 kilohertz. A Listen chip plays the tone; nothing plays until it is clicked, and the slider retunes it while it sounds. infrasound audible ultrasound f (Hz) 10 100 1000 10 000 100 000 20 20 000 f = 1.0 kHz, λ = 34.0 cm in air
SimSet a frequency with the slider, as a power of ten, from \(20\,\text{Hz}\) to \(20\,\text{kHz}\). The dot marks it on a logarithmic frequency axis, with the bands of infrasound, audible sound and ultrasound. The readout gives the wavelength in air at \(340\,\text{m/s}\). Press Listen, then move the slider while the tone plays.

Press Listen in the figure above and slide the frequency up slowly. Many adults stop hearing the tone somewhere between \(15\) and \(18\,\text{kHz}\), because the upper limit falls with age. At the low end, small speakers cannot produce the deepest tones well. The wavelengths in air run from \(340/20 = 17\,\text{m}\) at the bottom of the range to \(1.7\,\text{cm}\) at the top.

CheckpointUnanswered

A dog whistle produces a sound of about \(25\,\text{kHz}\). What kind of sound is this for a human listener?

CheckpointUnanswered

Elephants call to each other over several kilometres with rumbles as low as \(15\,\text{Hz}\). What kind of sound is this for a human listener?

In the world
Seeing with ultrasound

A hospital ultrasound scanner sends pulses of a few megahertz into the body and listens for their echoes. At \(3\,\text{MHz}\) the wavelength in soft tissue, where sound travels at about \(1500\,\text{m/s}\), is only half a millimetre. Such short waves reflect from small structures, so the echoes draw a picture of a baby in the womb. Bats use the same idea at about \(20\) to \(100\,\text{kHz}\) to hunt insects in the dark.

Thresholds of hearing and of pain
Maths you need

The range of intensities

The faintest sound that can be heard under ideal conditions has an intensity of about \(I_0 = 1.0 \times 10^{-12}\,\text{W/m}^2\). This corresponds to \(0\,\text{dB}\) on the decibel scale and is known as the threshold of hearing. It is the reference intensity of lesson 4.

At the other extreme, an intensity of order \(1\,\text{W/m}^2\), around \(120\,\text{dB}\), marks the threshold of pain. Prolonged exposure to sound levels near this intensity can permanently damage hearing. The ear spans a factor of \(10^{12}\) in intensity between these two thresholds.

The perception of sound is therefore shaped by two things. One is how much power per unit area reaches the ear, the intensity. The other is whether that power lies within the audible frequency band. A very intense sound at \(30\,\text{kHz}\) is still unheard.

Deeper

The threshold of hearing depends on the frequency. \(I_0 = 10^{-12}\,\text{W/m}^2\) is the value near \(1\) to \(4\,\text{kHz}\), where the ear is most sensitive. At \(50\,\text{Hz}\) a tone must be tens of decibels more intense to be heard at all. That is why a sound meter often uses a weighting, marked dB(A), which counts low and very high frequencies for less.

CheckpointUnanswered

Which of these sounds can a healthy young listener hear?

A ladder of common sound levels
Maths you need

Common sound levels

Here are some common sound levels, from the faintest to the most dangerous.

  • 0 dB: threshold of hearing
  • 30 dB: whisper
  • 60 dB: normal conversation
  • 90 dB: heavy traffic
  • 120 dB: threshold of pain
  • 140 dB: jet engine at close range
A ladder of sound levelsA vertical ladder of six rungs, placed by their sound level. From the bottom: threshold of hearing, 0 decibels, 10 to the minus 12 watts per square metre; whisper, 30 decibels, 10 to the minus 9; normal conversation, 60 decibels, 10 to the minus 6; heavy traffic, 90 decibels, 10 to the minus 3; threshold of pain, 120 decibels, 1 watt per square metre; jet engine at close range, 140 decibels, 100 watts per square metre. The level is written on each rung, the intensity to its left and the name to its right. Each step of 30 decibels multiplies the intensity by 1000. I (W/m²) β 0 dB 10⁻¹² threshold of hearing 30 dB 10⁻⁹ whisper 60 dB 10⁻⁶ normal conversation 90 dB 10⁻³ heavy traffic 120 dB 1 threshold of pain 140 dB 10² jet engine
Fig 5.1Common sound levels and their intensities. Each step of 30 dB on the ladder multiplies the intensity by 1000. The threshold of pain, 120 dB, is one million million times the threshold of hearing.

Read the ladder of Fig 5.1 in steps. From a whisper to normal conversation is \(30\,\text{dB}\), a factor of \(10^3\) in intensity. From conversation to heavy traffic is another \(10^3\). The jet engine at \(140\,\text{dB}\) delivers \(100\,\text{W/m}^2\), a hundred times the threshold of pain.

Distance and level

The level of a sound falls as you move away from it. For a point source the intensity falls as \(1/r^2\), by the inverse-square law of lesson 3. Each doubling of the distance divides the intensity by \(4\), a fall of \(10\log_{10}4 = 6\,\text{dB}\). Ten times the distance divides it by \(100\), a fall of \(20\,\text{dB}\).

CheckpointUnanswered

If the distance from a point source is tripled, the intensity

Checkpoint · numericUnanswered

A truck horn gives a sound level of \(90\,\text{dB}\) at \(2\,\text{m}\). Treat it as a point source in open air. What is the level at \(20\,\text{m}\), in dB?

dB± 2 %
In the world
Noise limits in India

The Noise Pollution (Regulation and Control) Rules of 2000 set limits on sound levels in India. In a residential area the limit is \(55\,\text{dB}\) by day and \(45\,\text{dB}\) at night. Near a hospital, school or court, a silence zone, it is \(50\,\text{dB}\) by day and \(40\,\text{dB}\) at night. The same rules forbid loudspeakers in the open between 10 p.m. and 6 a.m., except in a few permitted cases.

Pitch loudness and quality
Maths you need

Pitch, loudness and quality

The ear tells apart three characteristics of a musical note. The first is pitch, how high or low the note sounds. It is set by the frequency, and a higher frequency gives a higher pitch. The second is loudness, how strong the note sounds. It is set mainly by the intensity, which the sound level in decibels measures.

The third is quality, also called timbre. A sitar and a flute can play the same note at the same loudness, and still you can tell them apart. Each instrument sounds the note with its own mix of harmonics. These are tones at whole-number multiples of the lowest frequency, \(f_1\), \(2f_1\), \(3f_1\) and so on. The mix gives the waveform its shape, and the ear hears that shape as the quality.

The same pitch with different qualitiesLeft: the pressure variation delta P of a musical sound against time over two periods of 220 hertz. Right: a bar chart of the strengths of its first five harmonics, 220, 440, 660, 880 and 1100 hertz. Three chips choose the mix. Pure tone: only the first harmonic, and the wave is a sine curve. All harmonics: the strengths 1, 0.5, 0.33, 0.25 and 0.2, and the wave is steep on one side, like a saw tooth. Odd harmonics only: the strengths 1, 0, 0.33, 0 and 0.2, and the wave has flat tops, like a square wave; this is the mix of a clarinet, a pipe closed at one end. The period, and so the pitch, is the same in all three. A Listen chip plays the chosen mix; nothing plays until it is clicked.OtΔP harmonics 1 2 3 4 5 the same pitch: 220 Hz
Fig 5.2Three sounds with the same pitch, \(220\,\text{Hz}\). Left: the pressure wave over two periods. Right: the strengths of the first five harmonics. A pure tone has only the first. The second chip adds all five, and the third keeps only the odd ones. Press Listen and change the chip: the pitch stays the same and the quality changes.

Listen to Fig 5.2 and change the chip. The period of the wave never changes, so the pitch stays the same. Only the shape changes, and with it the quality. The pure tone sounds dull, like a tuning fork. The odd harmonics sound hollow, like a clarinet. A clarinet is a pipe closed at one end, and such a pipe cannot sound the even harmonics. The chapter Standing Sound Waves shows why.

CheckpointUnanswered

A sitar and a flute play the same note at the same sound level. You can still tell which is which. In what do the two sounds differ?

Now return to the dog whistle. It was loud enough, well above the threshold of hearing. But its frequency lay above \(20\,\text{kHz}\), outside the audible band of a human ear. A dog hears up to about \(45\,\text{kHz}\), so for the dog it was a clear call.

Exam traps
  1. Thinking a very intense sound must be audible.
    Its frequency must also lie between \(20\,\text{Hz}\) and \(20\,\text{kHz}\).
  2. Mixing up infrasound and ultrasound.
    Infrasound is below \(20\,\text{Hz}\); ultrasound is above \(20\,\text{kHz}\).
  3. Taking the level to fall in proportion to distance.
    For a point source, each doubling of distance lowers the level by \(6\,\text{dB}\), and ten times the distance by \(20\,\text{dB}\).
  4. Linking quality to loudness.
    Quality is set by the mix of harmonics. Two sounds of the same pitch and loudness can differ in quality.