Physics 2Waves, Sound and Physical Optics

Sound Intensity and Decibels

Intensity falls off as 1/r², and β = 10 log(I/I₀), so adding 10 dB means 10 times the intensity.

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In Sound: Pitch and Loudness, loudness came from amplitude. Physics measures it as intensity, power per area. Your ears handle a range of intensities of about a trillion to one, so we squeeze that range with What a Logarithm Is.

Key idea

A source of power $P$ spreading in all directions gives $I = \dfrac{P}{4\pi r^{2}}$ at distance $r$. The sound level is $$\beta = 10\log_{10}\frac{I}{I_0}\ \text{dB}, \qquad I_0 = 10^{-12}\ \text{W/m}^2.$$ Every $+10\ \text{dB}$ means $10$ times the intensity; $+3\ \text{dB}$ is about double.

Why it works

The power spreads over a sphere of area $4\pi r^{2}$, so twice as far means four times the area and a quarter of the intensity. For decibels: $\log_{10}$ turns multiplying into adding. Multiply $I$ by 10 and $\log_{10}(I/I_0)$ goes up by 1, so $\beta$ goes up by 10. Multiply by 2 and $\beta$ goes up by $10\log_{10}2 = 3.0\ \text{dB}$. $I_0$ is roughly the faintest sound a young ear can hear, so $0\ \text{dB}$ is the threshold of hearing, not silence.

Common mistake

Thinking that doubling the intensity doubles the decibel level. Two identical $60\ \text{dB}$ speakers give $63\ \text{dB}$, not $120\ \text{dB}$. Check: $120\ \text{dB}$ is a million times $60\ \text{dB}$ in intensity, far more than two speakers can add.

Worked example: From intensity to decibels

A sound has intensity $1.0 \times 10^{-5}\ \text{W/m}^2$. Find its level.
  1. $\dfrac{I}{I_0} = \dfrac{10^{-5}}{10^{-12}} = 10^{7}$.
  2. $\beta = 10\log_{10}(10^{7}) = 10(7) = 70\ \text{dB}$.

Answer: $70\ \text{dB}$

Worked example: Moving away

You hear a small speaker at $80\ \text{dB}$ from $2.0\ \text{m}$ away. What level do you hear at $20\ \text{m}$?
  1. Ten times as far gives $\frac{1}{10^{2}} = \frac{1}{100}$ of the intensity.
  2. Dividing by 100 is two factors of 10: $-20\ \text{dB}$.
  3. $80 - 20 = 60\ \text{dB}$.

Answer: $60\ \text{dB}$

Worked example: Power of a source

At $5.0\ \text{m}$ from a source the intensity is $2.0 \times 10^{-4}\ \text{W/m}^2$. What power does it put out as sound?
  1. $$P = I \cdot 4\pi r^{2} = (2.0 \times 10^{-4})(4\pi)(5.0)^{2}.$$
  2. $P = 0.063\ \text{W}$. Sound carries surprisingly little power.

Answer: $0.063\ \text{W}$

Sound is a pressure wave: the bigger the pressure swings, the more power each square meter receives.

Practice

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Builds on

Leads to

This is one of the top rungs of Physics 2: Fluids, Heat, Electricity, Light and Atoms.

Sources and further reading

  • OpenStax College Physics 2e, Section 17.3: Sound Intensity and Sound Level
  • OpenStax University Physics Volume 1, Section 17.3: Sound Intensity
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