But wait.  The actors can barely be heard!  The orchestra is drowning out their words!  All of a sudden the audience hears the air conditioning units coming on, a ventilation grille is rattling, and you can hear the people in the control room talking!  The audience is getting  restless and some patrons start to leave before the first act is even completed!  How could this disaster have been avoided?

The Acoustical Goals in Live Theatre Formats

The basic shape of the theatre can have an impact on the acoustics.  Some shapes  work and some don’t.  You may not be able to change the shape of an existing building, such as a historic restoration, or one that was designed without considering the acoustical impact of the dimensions,  but it is still possible to better the conditions while working within these parameters.

There are several acoustical goals when planning for multi-purpose theatres.  First, you must provide enough reverberation for the blending of musical performances while still maintaining high levels of speech  intelligibility  for drama and other spoken events.  One option to achieve this is through the use of diffusing panels.

Diffusion is extremely important in rooms used for musical performances. When good diffusion has been achieved, listeners have the sensation of being enveloped in sound. The  second acoustical goal is the control of noise from the building’s mechanical system (HVAC fan noise, for example) whose noise should be prevented from impacting the theatre.  A theatre has to be protected from mechanical noise so the theatre is ideally  located as  far away from the mechanical unit  as possible.  The remainder of the duct work should be treated with acoustical lining to further reduce the fan noise.

Speech intelligibility is greatly affected by reverberation.  The optimum reverberation time for speech auditoriums vary greatly from churches to opera houses to studios. 

The lower reverberation times for speech auditoriums demonstrate the influences of reverberation on speech intelligibility.  The rate at which the reverberant sound dies away is measured by the reverberation time, defined as the time required for the reverberant sound to diminish by 60 dB.  The reverberation time can be calculated approximately from the formula, T = 0.05 V/A, where V is the room volume, and A is the absorption in sabins, a sabin being the absorption of a square  foot  of  perfect absorber. 

Certain values of reverberation time have been found acceptable for various applications: for speech the middle-frequency reverberation time should be about one second or less; for solo instruments and chamber music, 1.0 to 1.5 sec; for symphonic music, 1.5 to 2.0 sec; for church music, 2.0 to 2.5 sec. Generally, longer times are accepted in larger halls and with larger musical ensembles. The time should be nearly constant with frequency, although for music a slight rise at low frequencies is desirable. 

What happens to a sound wave when it reaches a surface depends upon the absorption  of the surface.  Surfaces such as concrete or masonry that are impermeable have absorption coefficients less than 0.05 and are regarded as almost  perfect reflectors. Other surfaces such as thin plywood and plasterboard may be reflective at middle and high frequencies, but may have absorption rates as high as 0.50, due to panel resonances, at low frequencies. 

On the other hand, a thin porous material mounted against a hard backing will be mainly reflective at low frequencies, but will increase in absorption efficiency with increasing frequency. Acoustical plaster, carpet and wood are typical examples of this type of surface. Draperies also tend to absorb mostly at high frequencies, being practically transparent at low frequencies.

To achieve a constant reverberation time, it usually is necessary to adjust particularly the low and middle-frequency absorption.  An efficient absorbing system in this range often consists of a slotted or perforated screen over a backspace containing porous material.  The backspace, the perforated surface and the absorptive material constitute a resonant system that can be tuned to whatever frequency range is desired. Some commercial acoustical materials combine two of the above features.

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