
The figure above shows measured frequency responses for two different
directions of arrival. In each case we see that there are two paths from
the source to the ear canal -- a direct path and a longer path following
a reflection from the pinna. At moderately low frequencies, the pinna essentially
collects additional sound energy, and the signals from the two paths arrive
in phase. However, at high frequencies, the delayed signal is out of phase
with the direct signal, and destructive interference occurs. The greatest
interference occurs when the difference in path length d is a half wavelength,
i.e., when f = c / 2d. In the example shown, this produces a "pinna
notch" around 10 kHz. With typical values for d, the notch
frequency is usually in the 6-kHz to 16-kHz range.
Since the pinna is a more effective reflector for sounds coming from the
front than for sounds from above, the resulting notch is much more pronounced
for sources in front than for sources above. In addition, the path length
difference changes with elevation angle, so the frequency of the notch moves
with elevation. Although there are still disputes about what features are
perceptually most important (for example, see Han),
it is well established that the pinna provides the primary cues for elevation.
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