The following is from The Funk & Wagnalls New Encyclopedia,
1994*
ACOUSTICS ( Gr. akouein, "to hear"),
term sometimes used for the science of sound in general, but
more commonly for the special branch of that science, architectural
acoustics, that deals with the construction of enclosed areas
so as to enhance the hearing of speech or music. For the treatment
of acoustics as a branch of the pure science of physics, see Sound
.
The acoustics of buildings was an undeveloped aspect of the study
of sound until comparatively recent times. The Roman architect
Marcus Pollio, who lived during the 1st century bc, made some
pertinent observations on the subject and some astute guesses
concerning reverberation and interference. The scientific aspects
of this subject, however, were first thoroughly treated by the
American physicist Joseph Henry in 1856 and more fully developed
by the American physicist Wallace Sabine (1868-1919) in 1900.
Problems of Design.
Acoustical design must take into consideration that in addition
to physiological peculiarities of the ear, hearing is complicated
by psychological peculiarities. For example, sounds that are unfamiliar
seem unnatural. Sound produced in an ordinary room is somewhat
modified by reverberations due to reflections from walls and furniture;
for this reason, a broadcasting studio should have a normal degree
of reverberation to ensure natural reproduction of sound. For
best acoustic qualities, rooms are designed to produce sufficient
reflections for naturalness, without introducing excessive reverberation
at any frequency, without echoing certain frequencies unnaturally,
and without producing undesirable interference effects or distortion.
The time required for a sound to diminish to one-millionth of
its original intensity is called reverberation time. An appreciable
reverberation time improves acoustical effect, especially for
music; a loud sound should still be barely audible for one to
two seconds after the sound has stopped in an auditorium. In a
private home a shorter but still discernible reverberation time
is desirable.
Materials.
For modifying the reverberations, the architect has two types
of materials, sound-absorbent and sound-reflecting, to coat the
surfaces of ceilings, walls, and floors. Soft materials such as
cork and felt absorb most of the sound that strikes them, although
they may reflect some of the low-frequency sounds. Hard materials
such as stone and metals reflect most of the sound that strikes
them. The acoustics of a large auditorium may be very different
when it is full from when it is empty; empty seats reflect sound,
whereas an audience absorbs sound.
In most cases, the acoustics of a room will be satisfactory if
a proper balance between sound-absorbing and sound-reflecting
materials is created. Troublesome echoes may frequently occur
in a room that otherwise has a proper overall reverberation time
if the ceiling or a wall is concave in shape and is highly reflecting;
in such cases, sound may be focused at a particular point, making
the acoustics bad at that point in the room. Similarly, a narrow
corridor between parallel reflecting walls may trap sound by repeated
reflection and cause troublesome echoes, even though the overall
absorption is sufficient. Attention must also be given to the
elimination of interference. Such interference arises from the
difference in the distances traversed by the direct and the reflected
sound and produces so-called dead spots, in which certain ranges
of frequency are canceled out. Reproduction of sound picked up
by microphones also requires the elimination of echoes and interference.
Insulation.
Another aspect of room acoustics is insulation from unwanted
sound. This is obtained by sealing even the smallest openings
that can leak sound, by using massive walls, and by building unconnected
walls separated by dead spaces.
To evaluate the acoustical properties of rooms and materials,
the acoustical scientist uses tools such as anechoic chambers
and sound-level meters. The anechoic chamber is a room free from
echoes and reverberations in which all sound is absorbed by glass-fiber
wedges placed on the surfaces of the walls. A sound-level meter
measures sound intensity, the rate of flow of sound energy, which
is related to the loudness of a sound, and expresses the result
in decibels (dB), a logarithmic unit. In a quiet residence the
sound-level meter would read about 38 dB. An ordinary conversation
would increase the sound-level reading to about 70 dB. The sound
intensity of an air-raid siren could reach about 150 dB; a jet-airplane
noise, around 120 dB. When perceived sound intensity is doubled,
its power level increases by 10 times, or 10 dB. Loudness levels,
which depend upon the judgment of the listener, are measured in
sones and phons.
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