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Oceans of noise - Whale and Dolphin Conservation Society

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2.1.2. Measuring sound intensity<br />

Ideally, acousticians would be able to measure intensity directly but practically it is easier to measure<br />

<strong>and</strong> detect changes in pressure <strong>and</strong> then convert these to intensities. However, the use <strong>of</strong> pressure as a<br />

measurement unit presents the acoustician with two problems, the first is related to the range <strong>of</strong><br />

pressure differences that the human auditory system can detect (10_Pa – 100,000,000_Pa) <strong>and</strong> the<br />

second is related to the way in which the human auditory system processes differences in pressure, i.e.<br />

how it judges relative loudness. The former is a practical problem where the magnitude <strong>of</strong> pressure<br />

differences detectable by the human ear can make calculations clumsy, <strong>and</strong> the latter is a subjective<br />

problem whereby the human auditory system processes pressure differences logarithmically <strong>and</strong><br />

judges these relatively. It is for these reasons that Decibel Scale <strong>and</strong> dimensionless unit the Decibel<br />

(dB) were introduced, <strong>and</strong> the terms Sound Pressure Level (SPL) <strong>and</strong> Sound Intensity Level (SIL)<br />

were defined.<br />

⎛ ⎞<br />

⎜<br />

p<br />

SPL( dB)<br />

= 20log<br />

⎟<br />

⎜ ⎟<br />

⎝ p dB ⋅ re.<br />

1µ<br />

Pa<br />

ref ⎠<br />

Where p is the measured pressure <strong>and</strong> pref is the reference pressure. In underwater acoustics pref water =<br />

1µPa, in air pref air = 20µPa<br />

⎛ ⎞<br />

⎜<br />

I<br />

SIL( dB)<br />

= 10log<br />

⎟<br />

⎜ ⎟<br />

⎝ I dB ⋅ re.<br />

1µ<br />

Pa<br />

ref ⎠<br />

Where I is the measured intensity <strong>and</strong> Iref is the reference intensity. Historically, the reference intensity<br />

(Iref) in air was the sound intensity barely audible to humans at 1000Hz, i.e. 1x10 -12 Wm -2 (1 pico Wm -<br />

2 ). Note that if both SPL <strong>and</strong> SIL are quoted in dB they are equivalent, i.e.<br />

⎛ I ⎞ ⎛ p ⎞<br />

SIL(<br />

dB)<br />

= 10log⎜<br />

⎟ = 20log⎜<br />

⎟ = SPL(<br />

dB)<br />

⎜ I ⎟ ⎜<br />

ref p ⎟<br />

⎝ ⎠ ⎝ ref ⎠<br />

From the definitions <strong>of</strong> SPL <strong>and</strong> SIL above it should be clear that decibel scale is a log ratio scale <strong>of</strong><br />

intensity that has dimensionless units – the decibel. It should also be clear that decibel scale<br />

overcomes the problems discussed above, (1) ratios are a convenient way <strong>of</strong> dealing with the large<br />

range <strong>of</strong> intensities (pressures) that the human ear can detect, (2) logarithms simplify computations<br />

since multiplication <strong>and</strong> division are reduced to addition <strong>and</strong> subtraction, <strong>and</strong> (3) the logarithmic scale<br />

approximates the mechanism by which the human auditory system judges relative loudness.<br />

It is important to note the dB scale is relative <strong>and</strong> that dB values are only meaningful if a reference<br />

level is included. The reference levels for SPL <strong>and</strong> SIL are equivalent but are reported in different<br />

units. In underwater acoustics a reference pressure <strong>of</strong> 1_Pa is commonly used, while the reference<br />

pressure in air is 20_Pa (this approximates the human hearing threshold at 1000Hz). The reference<br />

intensity in water can be calculated from reference pressure by:<br />

I<br />

ref<br />

⎛<br />

= ⎜<br />

⎝ ( ρ<br />

p<br />

c<br />

medium<br />

2<br />

ref<br />

medium<br />

⎞<br />

⎟<br />

) ⎟<br />

⎠<br />

19

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