Search

Google Website Translator Gadget

Sunday, February 20, 2011

Basic requirements for an acoustically good hall

1. Reflection

In completely free space, sounds travel outwards from their source with diminishing intensity until all the energy has been dissipated in the ever-widening wavefront or lost as heat in the air itself. By contrast, sound waves in a concert hall are repeatedly turned back on themselves and bounced in criss-cross patterns throughout the enclosed space. The audience therefore hears not only the direct sound but also a mixture of later—and weaker—sounds. These multiple reflections are delayed in accordance with the extra distance travelled; and they diminish in intensity through normal dissipation and absorption at each boundary reflection.
A near-perfect reflector such as a polished wood floor will reflect almost 100 per cent of the incident energy, but soft furnishings, porous fibre-tiles, or pliant panels will absorb part of that energy. In practice, the different kinds of absorber are frequency-selective, and good acoustic design depends on careful disposition of various absorbers to control reflections evenly at bass, middle, and treble frequencies.

2. Directional effects

Sound sources are described as directional or non-directional depending on whether they are physically large or small compared with the wavelength of the musical notes being radiated (see acoustics, 10). For similar reasons, reflectors of different sizes and shapes may modify the distribution, i.e. diffusion, of sounds throughout a room not only by frequency-selective reflection but also by re-radiating some bands of frequencies uniformly and others in a directional manner. If curved surfaces are essential, a convex shape is generally preferred because it tends to scatter sounds and help produce uniform listening conditions. Concave surfaces focus sounds back along their axis and give rise to local echoes or dead spots.
A domed ceiling is a classic example of the concave shape to be avoided. The Royal Albert Hall in London is perhaps specially unfortunate in having both an oval plan and a high domed ceiling focusing sounds on to parts of the audience area. The effects of marked echoes were complained of for many years until arrays of ‘flying saucers’ were suspended beneath the huge dome. The underside of the saucers is convex, to scatter the upward-travelling sound waves, and their tops carry absorbent material to capture any sounds that missed the saucers on the way up and rebounded from the ceiling. In the same way, recesses or coffering should be of generous proportions so that their scattering effect will be felt through most of the frequency spectrum.

3. Reverberation

Although members of an audience receive the direct sound followed by a wedge or ‘tail’ of countless reflected waves, they are not normally conscious of these as separate entities or echoes. The hearing mechanism (see ear and hearing) works in such a way that sound repetitions arriving within about 1/20; of a second of each other are run together and heard as one. Note, however, that ‘flutter echoes’ can arise between parallel walls.
The prolongation effect is known as ‘reverberation’. A smooth decay is to be preferred, secured by careful acoustic design to produce evenly diffused sounds. The time taken for sounds to fall to inaudibility is called the ‘reverberation time’ (strictly the time to fall to a millionth of its original value, or to −60 dB). Reverberation time increases in direct proportion to the volume (size) of the enclosure—the greater distances stretching the decay period—but is reduced by the introduction of absorbent materials. An audience also mops up sound energy quite effectively, so rehearsals in an empty hall sound much more reverberant than the actual concert. To reduce this difference, modern concert-hall seating can be designed so that each seat absorbs about the same amount of sound whether occupied or not.

4. Designing for good acoustics

For speech, the principal criteria for design are adequate loudness and a high degree of intelligibility. This suggests a short reverberation time; yet too dry an acoustic will lack the reflected energy needed to carry adequate sound levels to listeners at greater distances from the platform. Attention to room shape and seating layout is necessary, and a sloping or raked floor will help to give listeners in the back row a clear view of the speakers and a better chance of hearing properly.
For music, there are additional acoustic requirements, making acoustic design as much art as science. From an examination of existing halls generally rated as having ‘good acoustics’, Leo L. Beranek, for example, listed 18 criteria of quality in his book Music, Acoustics and Architecture. Historically, increasingly large halls have been built, with correspondingly greater reverberation times, as the size of orchestras has grown. Thus Baroque and chamber music are suited to a reverberation time of less than 1.5 seconds, Classical music about 1.7, and Romantic music about 2.2 seconds. A longer decay at low frequencies makes for fullness of tone or warmth, whereas good definition or clarity demands a rise at high frequencies.
Modern concert halls often incorporate some means of varying the reverberation characteristics to suit different musical or non-musical events. A good example is Symphony Hall in Birmingham (opened in 1991 ) where a movable circular canopy over the platform area directs sound towards specific regions of the auditorium, and reverberation chambers round the periphery can be opened to increase reverberation time.
Performing musicians naturally demand a sense of ease and power in producing adequate tone without fatigue. This is helped by strategic placing near the players of reflecting surfaces which also enable them to hear each other clearly. There seems no doubt that composers of all periods consciously or unconsciously wrote in such a way as to suit the environment in which their music would be performed.

5. Problems of small rooms

In the reverberant sound field of a large hall, the random streams of reflected sound waves produce a reasonably consistent diffusion of sound. In small rooms, however, distinct interference patterns are set up by multiple reflections between parallel walls, floor, and ceiling. These ‘standing wave’ resonances, which form a kind of three-dimensional organ-pipe effect, occur at frequencies of which the distances between the parallel surfaces are multiples of a half-wavelength. A harmonic series of these room resonances, or ‘eigentones’, exists for each room dimension, and the uneven boosting of certain frequencies causes coloration of the sound. Selective bass absorption is needed, or a special design using non-parallel walls.

6. Sound reinforcement

It is economically impossible to limit the use of most halls to musical forces of optimum size and acoustic power. The question of amplification then arises for quiet instruments or voices. In many churches and lecture theatres, the building shape or shortcomings in the acoustic distribution call for augmentation of the natural sounds, either overall or selectively in particular areas. The basic components for sound reinforcement or ‘public address’ are a microphone, amplifier, and loudspeaker. The arrangement is inherently unstable, however, as most users can testify, since any amplified sound from the loudspeaker that falls on the microphone is again amplified and sent to the loudspeaker with the possibility of uncontrolled feedback. Directional microphones can ease the problem since their less sensitive side(s) can be directed towards the loudspeaker(s) and so reduce unwanted pickup of the amplified sound. Directional loudspeaker arrays can also beam the sound waves into specific areas to give more efficient reinforcement without feedback.

7. Assisted resonance

A special kind of sound reinforcement, called assisted resonance, is used in some halls to increase the reverberation time within certain frequency bands. A classic example is the Royal Festival Hall in London, where the original 1948 design had called for a reverberation period of 1.7 seconds, rising to 2.5 seconds at low frequencies. When the hall was built, however, the low-frequency reverberation time measured only 1.4 seconds and, while this gave excellent definition, the hall was criticized as lacking fullness of tone. In 1964 matters were improved by assisted resonance using 172 microphones at roof level, amplifiers tuned to narrow frequency bands in the range 58–700 Hz, and arrays of loudspeakers.

8. Sound insulation

A requirement in every type of auditorium is for the lowest practical level of extraneous noise, whether airborne or transmitted through the structure of the building. A first step in planning is to choose a quiet site—not very practicable in a large city—and to design the building with as many layers or shells as possible on the side nearest to railway lines or other identifiable sources of noise. Aircraft noise is an increasing problem requiring the use of massive roofs on insulating supports, with suspended ceilings, floating floors, and multi-layered exterior walls. The Bridgewater Hall in Manchester (opened in 1996 ) has achieved almost total exclusion of external noise. Its massive 22,500-tonne weight is suspended on some 300 isolation spring bearings, and its three-layer roof has an outer sheet of steel lined with acoustic panels.

0 comments: