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Introduction to Acoustics

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Absolute threshold (dB SPL)<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

–20<br />

0<br />

20<br />

40<br />

60<br />

80<br />

100<br />

120<br />

0.125 0.25 0.5 1 2 4 8<br />

Frequency (kHz)<br />

Hearing level (dB HL)<br />

0.125<br />

0.25 0.5 1 2 4 8<br />

Frequency (kHz)<br />

Fig. 13.2 Comparison of a clinical audiogram for a 50 dB<br />

hearing loss at all frequencies (bot<strong>to</strong>m) and the absolute<br />

threshold curve for the same hearing loss plotted in terms<br />

of the MAP (<strong>to</strong>p)<br />

suspected; thresholds are specified relative <strong>to</strong> the average<br />

threshold at each frequency for young, healthy listeners<br />

13.2 Frequency Selectivity and Masking<br />

Frequency selectivity refers <strong>to</strong> the ability <strong>to</strong> resolve or<br />

separate the sinusoidal components in a complex sound.<br />

It is a key aspect of the analysis of sounds by the audi<strong>to</strong>ry<br />

system, and it influences many aspects of audi<strong>to</strong>ry perception,<br />

including the perception of loudness, pitch and<br />

timbre. It is often demonstrated and measured by studying<br />

masking, which has been defined as ‘The process by<br />

which the threshold of audibility for one sound is raised<br />

Psychoacoustics 13.2 Frequency Selectivity and Masking 461<br />

with normal hearing. In this case, the sound level is usually<br />

specified relative <strong>to</strong> standardized values produced<br />

by a specific earphone in a specific coupler. A coupler is<br />

a device which contains a cavity or series of cavities and<br />

a microphone for measuring the sound produced by the<br />

earphone. The preferred earphone varies from one country<br />

<strong>to</strong> another. For example, the Telephonics TDH49 or<br />

TDH50 is often used in the UK and USA, while the<br />

Beyer DT48 is used in Germany. Thresholds specified<br />

in this way have units of dB HL (hearing level) in Europe<br />

or dB HTL (hearing threshold level) in the USA.<br />

For example, a threshold of 40 dB HL at 1 kHz would<br />

mean that the person had a threshold which was 40 dB<br />

higher than normal at that frequency. In psychoacoustic<br />

work, thresholds are normally plotted with threshold<br />

increasing upward, as in Fig. 13.1. However, in audiology,<br />

threshold elevations are shown as hearing losses,<br />

plotted downward. The average normal threshold is represented<br />

as a horizontal line at the <strong>to</strong>p of the plot, and<br />

the degree of hearing loss is indicated by how much the<br />

threshold falls below this line. This type of plot is called<br />

an audiogram. Figure 13.2 compares an audiogram for<br />

a hypothetical hearing-impaired person with a flat hearing<br />

loss, with a plot of the same thresholds expressed<br />

as MAP values. Notice that, although the audiogram is<br />

flat, the corresponding MAP curve is not flat. Note also<br />

that thresholds in dB HL can be negative. For example,<br />

a threshold of −10 dB simply means that the individual<br />

is 10 dB more sensitive than the average.<br />

The absolute thresholds described above were measured<br />

using <strong>to</strong>ne bursts of relatively long duration. For<br />

durations exceeding about 500 ms, the sound level at<br />

threshold is roughly independent of duration. However,<br />

for durations less than about 200 ms, the sound level necessary<br />

for detection increases as duration decreases, by<br />

about 3 dB per halving of the duration [13.9]. Thus, the<br />

sound energy required for threshold is roughly constant.<br />

by the presence of another (masking) sound’ [13.10]. It<br />

has been known for many years that a signal is most<br />

easily masked by a sound having frequency components<br />

close <strong>to</strong>, or the same as, those of the signal [13.11]. This<br />

led <strong>to</strong> the idea that our ability <strong>to</strong> separate the components<br />

of a complex sound depends, at least in part, on<br />

the frequency analysis that takes place on the basilar<br />

membrane (see Chap. 12).<br />

Part D 13.2

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