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<H1>Classroom Acoustics</H1>
<P><IMG src=3D"http://asa.aip.org/classroom/cover.jpg"></CENTER>
<P>The intent of this publication is to create a supplemental resource =
for=20
architects, educators, and school planners for use with new construction =
or=20
renovation of learning environments. The publication is not intended to =
replace=20
the services of a professional acoustical consultant. It is to be used =
as an aid=20
in the understanding of the elements of desirable listening conditions =
in=20
classrooms.=20
<P>This publication was prepared for the Technical Committee on =
Architectural=20
Acoustics of the Acoustical Society of America by Benjamin Seep, Robin=20
Glosemeyer, Emily Hulce, Matt Linn, and Pamela Aytar who, at the time of =

publication preparation, were senior students in the Architectural =
Engineering=20
program at the University of Kansas. Supervision of this endeavor was =
provided=20
by Bob Coffeen, FASA, a member of the the University of Kansas =
Architectural=20
Engineering faculty.=20
<P>This publication was printed in August, 2000.=20
<P>
<HR>

<P>
<H3>INTRODUCTION</H3>
<P>The United States is currently in the midst of the largest campaign =
of school=20
construction and renovation in history. With the increased emphasis on=20
education, we must seize the opportunity to end a long-standing American =

practice: the building of classrooms with inferior acoustics. This =
invisible=20
problem has far-reaching implications for learning, but is easily =
solved.=20
<P>Excessive noise and reverberation interfere with speech =
intelligibility,=20
resulting in reduced understanding and therefore reduced learning. In =
many=20
classrooms in the United States, the speech intelligibility rating is 75 =
percent=20
or less. That means that, in speech intelligibility tests, listeners =
with normal=20
hearing can understand only 75 percent of the words read from a list. =
Imagine=20
reading a textbook with every fourth word missing, and being expected to =

understand the material and be tested on it. Sounds ridiculous? Well, =
that is=20
exactly the situation facing students every day in schools all across =
the=20
country.=20
<P>Many educators feel it is important to improve acoustics in =
classrooms used=20
by children with hearing problems, but unnecessary to do so in those =
used by=20
students with normal hearing. Yet many populations of students with =
"normal=20
hearing" also benefit from better classroom acoustics. These include =
students=20
with learning disabilities, those with auditory processing problems, and =
those=20
for whom English is a second language. Often, such students are not =
placed in=20
separate classrooms with enhanced acoustics, but are main-streamed with =
other=20
students. Another group for whom learning is especially dependent on =
good=20
acoustics is young children, who are unable to "predict from context." =
With=20
their limited vocabulary and experience, if they miss a few words from a =

teacher=92s lecture, they are less able than older students to "fill in" =
the=20
missing thoughts. Given these considerations, it is clear that a wide =
range of=20
students benefit from improved classroom acoustics.=20
<P>Why should classroom acoustics problems be endemic, when solutions =
are not=20
prohibitively expensive? The main reason is not lack of funds, but lack =
of=20
awareness of the problem and its solutions. In 1998, an incredible $7.9 =
billion=20
was spent on school buildings nationwide. For only a fraction more, all =
these=20
spaces could have been designed or renovated to provide good listening=20
conditions. For this to happen, however, school planners and architects =
must=20
begin the design process with classroom acoustics in mind. The best way =
to solve=20
acoustics problems is to prevent them beforehand, not correct them after =
the=20
fact. During the design process, acoustics problems can usually be =
avoided with=20
a bit of forethought and a different arrangement of the same building =
materials.=20
Renovation of poorly designed classrooms is much more expensive. Even =
then, the=20
cost of renovation is small compared to the social costs of poor =
classroom=20
acoustics that impair the learning of millions of children.=20
<P>The need for good classroom acoustics and the methods for attaining =
them have=20
been known for decades, but this information has not been made readily =
available=20
to architects, school planners, administrators, teachers, and parents. =
This=20
booklet is designed to provide a general overview of the problems and =
solutions=20
concerning classroom acoustics for both new construction and renovation. =

Straightforward, practical explanations and examples are given in the =
text; the=20
Appendix provides quantitative definitions and calculations, as well as=20
resources for more detailed information. The design of spaces with =
special=20
acoustical requirements, such as theaters or music rooms, or any spaces =
with=20
complex noise problems, are best handled by a professional acoustical=20
consultant.=20
<P>
<H3>THE BASICS</H3>
<P>We often talk about wanting to build rooms with "good acoustics," but =
this=20
has become a vague and almost meaningless term. There is no single,=20
all-encompassing set of criteria that will yield "good acoustics" for =
all rooms=20
and uses. Small classrooms, large lecture rooms, auditoriums, music =
rooms,=20
cafeterias, and gymnasiums all have different acoustical requirements. =
To=20
understand how these different spaces should be designed, we must first=20
familiarize ourselves with a few basic properties of sound.=20
<P>In the first century B.C., the Roman architect Vitruvius explained in =
De=20
architectura, his famous 10-volume treatise on architecture, that sound =
"moves=20
in an endless number of circular rounds, like the innumerably increasing =

circular waves which appear when a stone is thrown into smooth water =85 =
but while=20
in the case of water the circles move horizontally on a plane surface, =
the voice=20
not only proceeds horizontally, but also ascends vertically by regular =
stages."=20
While Vitruvius did not understand everything about sound, he was =
correct about=20
this particular point. In general, sound radiates in waves in all =
directions=20
from a point source until it encounters obstacles like walls or =
ceilings. Two=20
characteristics of these sound waves are of particular interest to us in =

architectural acoustics: <B>intensity</B> and <B>frequency</B>. =
Intensity is a=20
physical measurement of a sound wave that relates to how loud a sound is =

perceived to be. We can also measure the frequency of a sound wave, =
which we=20
perceive as pitch. For example, on a piano, the keys to the right have a =
higher=20
pitch than those to the left. If a sound has just one frequency, it is =
called a=20
pure tone, but most everyday sounds like speech, music, and noise are =
complex=20
sounds composed of a mix of different frequencies. The importance of =
frequency=20
arises when a sound wave encounters a surface: the sound will react =
differently=20
at different frequencies. The sensitivity of the human ear also varies =
with=20
frequency, and we are more likely to be disturbed by medium-to =
high-frequency=20
noises, especially pure tones.=20
<P>Think of sound as a beam, like a ray of light, passing through space =
and=20
encountering objects. When sound strikes a surface, a number of things =
can=20
happen, including: <B>Transmission</B>-- The sound passes through the =
surface=20
into the space beyond it, like light passing through a window.=20
<B>Absorption</B>-- The surface absorbs the sound like a sponge absorbs =
water.=20
<B>Reflection</B>-- The sound strikes the surface and changes direction =
like a=20
ball bouncing off a wall. <B>Diffusion</B>-- The sound strikes the =
surface and=20
is scattered in many directions, like pins being hit by a bowling ball. =
(See=20
Figure 1.) Keep in mind that several of these actions can occur =
simultaneously.=20
For instance, a sound wave can, at the same time, be both reflected by =
and=20
partially absorbed by a wall.=20
<P>
<CENTER><IMG =
src=3D"http://asa.aip.org/classroom/soundsurface.jpg"></CENTER>
<P>As a result, the reflected wave will not be as loud as the initial =
wave. The=20
frequency of the sound also makes a difference. Many surfaces absorb =
sounds with=20
high frequencies and reflect sounds with low frequencies. The =
<B>Absorption=20
Coefficient</B> ( a) and <B>NRC</B> (noise reduction coefficient) are =
used to=20
specify the ability of a material to absorb sound.=20
<P>A special problem that results from reflected sound is that of =
<B>discrete=20
echoes</B>. Most people are familiar with the phenomenon of shouting =
into a=20
canyon and hearing one=92s voice answer a second later. Echoes can also =
happen in=20
rooms, albeit more quickly. If a teacher=92s voice is continuously =
echoing off the=20
back wall of a classroom, each echo will interfere with the next word, =
making=20
the lecture difficult to understand. Echoes are also a common problem in =

gymnasiums.=20
<P>Another type of echo that interferes with hearing is <B>flutter =
echo</B>.=20
When two flat, hard surfaces are parallel, a sound can rapidly bounce =
back and=20
forth between them and create a ringing effect. This can happen between =
two=20
walls, or a floor and ceiling.=20
<P>Sound intensity levels and sound pressure levels can be measured in=20
<B>decibels (dB)</B>. In general, loud sounds have a greater dB value =
than soft=20
sounds. Because the decibel scale is logarithmic rather than linear, =
decibels=20
can not be added in the usual way.=20
<P>An important acoustical measurement called <B>Reverberation Time</B>=20
(<B>RT</B> or <B>RT(60)</B>) is used to determine how quickly sound =
decays in a=20
room. Reverberation time depends on the physical volume and surface =
materials of=20
a room. Large spaces, such as cathedrals and gymnasiums, usually have =
longer=20
reverberation times and sound =93lively=94 or sometimes =93boomy.=94 =
Small rooms, such=20
as bedrooms and recording studios, are usually less reverberant and =
sound =93dry=94=20
or =93dead.=94=20
<P>The <B>Noise Reduction (NR)</B> of a wall (also expressed in dB) =
between two=20
rooms is found by measuring what percentage of the sound produced in one =
room=20
passes through the wall into the neighboring room. (See Figure 2.) The =
NR is=20
calculated by subtracting the noise level in dB in the receiving room =
from the=20
noise level in the source room.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/wall.jpg"></CENTER>
<P><B>Signal-to-Noise Ratio (S/N)</B> is a simple comparison that is =
useful for=20
estimating how understandable speech is in a room. The sound level of =
the=20
teacher=92s voice in dB, minus the background noise level in the room in =
dB,=20
equals the S/N in dB. The larger the S/N, the greater the speech=20
intelligibility. If the S/N is negative (i.e., the background noise is =
louder=20
than the teacher=92s voice), the teacher will be hard to understand. =
Note also=20
that the S/N varies throughout the room as the signal and noise levels =
vary.=20
Typically, the S/N is lowest either: (1) at the back of the classroom, =
where the=20
level of the teacher=92s voice has fallen to its minimum value; or (2) =
near the=20
noise source, where the noise level is at its maximum, such as near a =
wall air=20
conditioning unit. Studies have shown that, in classrooms having a =
signal-to-=20
noise ratio of less than +10 dB, speech intelligibility is significantly =

degraded for children with average hearing. Children with some hearing=20
impairment need at least a +15 dB S/N ratio.=20
<P><B>Speech intelligibility</B> can be evaluated in existing rooms by =
using=20
<B>word lists</B>. Several tests are performed wherein one person =
recites words=20
from a standard list, and listeners write down what they hear. The =
percentage of=20
words listeners correctly hear is a measure of the room=92s speech=20
intelligibility.=20
<P>For those interested in learning more about these topics, additional=20
information is provided in the Appendix.=20
<P>
<H2>ACOUSTICAL GUIDELINES FOR CLASSROOMS</H2>
<P>Now that we have familiarized ourselves with these fundamentals of =
acoustics,=20
we can learn how to apply them to achieve satisfactory hearing =
conditions in=20
classrooms. The following guidelines are designed for a typical =
classroom of=20
approximately 30 students, where lecturing is done from the front of the =
room or=20
students work in small groups. Recommendations for gymnasiums, =
cafeterias, and=20
auditoriums are given in a following section.=20
<H3>REVERBERATION</H3>Though long reverberation time (RT) is the =
=93common cold=94=20
of bad classroom acoustics, there is a cure. Ideally, classrooms should =
have RTs=20
in the range of 0.4-0.6 seconds, but many existing classrooms have RTs =
of one=20
second or more. Figure 3 gives suitable reverberation times for various =
rooms=20
typically found in educational facilities. The RT can be estimated =
fairly easily=20
for both built and unbuilt classrooms with the use of the Sabine =
equation (see=20
page 10). The variables are the physical volume (ft 3 ) of the room, the =
areas=20
(ft 2 ) of different surface materials, and the absorption coefficients =
of those=20
materials at certain frequencies. The absorption coefficient is a =
measure how=20
much of the energy of a sound wave a material will absorb.=20
<P>There are two ways to reduce the RT of a room: either the volume must =
be=20
decreased or the sound absorption must be increased. Though decreasing =
the=20
volume is not always an option, it is a viable alternative for many =
older=20
classrooms with high ceilings. In such spaces, adding a suspended =
ceiling of=20
sound-absorbing tile can significantly improve the acoustics by =
simultaneously=20
decreasing the volume and increasing absorption. However, adding a =
suspended=20
ceiling often requires new light fixtures and can interfere with tall =
windows.=20
The case study presented later shows an alternative solution for =
classrooms with=20
high ceilings.=20
<P>Increasing the absorption in a room is accomplished by adding more =
=93soft=94=20
materials, such as fabric-faced glass fiber wall panels, carpet, or =
acoustical=20
ceiling tiles. Many products are commercially available for this =
purpose, and -=20
with forethought - it is possible to design a classroom with an =
acceptable RT=20
using common building materials. Absorptive materials work best when =
spread=20
throughout the room and not concentrated on just one wall or the floor =
or=20
ceiling. In many classrooms, a suspended ceiling of acoustical ceiling =
tiles=20
alone will decrease reverberation time to the desired range; however, =
this will=20
not address the problem of echoes from the walls. Nor are all =
=93acoustical=94=20
ceiling tiles created equal. Check the specifications and look for =
ceiling tiles=20
with an NRC of 0.75 or better. In order to absorb both low- and =
high-frequency=20
sounds, it is necessary to suspend the ceiling below the structural =
ceiling.=20
Simply adding carpeting to a classroom floor will not significantly =
reduce=20
reverberation time, especially at low frequencies, but carpeting will =
reduce=20
noise resulting from students sliding their chairs or desks on the =
floor.=20
<P>For those interested in calculating the RT of an existing classroom =
or=20
estimating how much absorption is necessary, the Appendix includes =
examples and=20
a table of absorption coefficients for some common materials.=20
<P>
<H3>UNDESIRABLE REFLECTIONS</H3>
<P>As mentioned above, echoes interfere with speech intelligibility. =
Echoes can=20
be controlled using absorption and/or diffusion. When locating =
absorptive=20
materials to reduce reverberation time, consider how they might help =
reduce=20
echoes as well. Placing an absorptive material on the rear wall of a =
classroom=20
prevents the teacher=92s voice from reflecting back to the front of the =
room.=20
While absorption is one way of minimizing reflected energy into the =
classroom,=20
another approach utilizes diffusion. Placing a diffusing element on the =
rear=20
wall of the classroom scatters the sound into many directions, so that =
the level=20
in any one particular direction is greatly reduced. Flutter echo is a=20
particularly significant problem when it occurs between the walls at the =
front=20
of the room where the teacher is speaking. A simple way to test whether =
flutter=20
echo is a problem is to stand near the center of the classroom, between =
parallel=20
surfaces, and clap hands once sharply. If flutter echo exists, a zinging =
or=20
ringing sound will be heard after the clap as the sound rapidly bounces =
back and=20
forth between two walls. Try turning in different directions and =
clapping again=20
to determine which walls are causing the flutter echo. To eliminate =
flutter echo=20
between two hard, parallel walls, cover one or both of them with =
fabric-faced=20
glass fiber panels or a similar sound-absorbing material. This works =
well if the=20
panels are staggered along the opposite walls so that a panel on one =
wall faces=20
an untreated surface on the opposite wall. Splaying two walls at least =
eight=20
degrees out of parallel will also eliminate flutter echo between them.=20
<P>
<H3>USEFUL REFLECTIONS</H3>
<P>So far we have discussed methods for reducing reflections in =
classrooms, but=20
in some cases we want to reinforce certain reflections. This is =
especially true=20
in large classrooms that have short reverberation times. The sound =
energy of the=20
teacher=92s voice can be absorbed by the soft ceiling before it reaches =
students=20
at the back of the room. The teacher=92s voice can be spread throughout =
the room=20
by shaping a sound-reflecting gypsum board ceiling over the front of the =
room,=20
or by making the center of the ceiling a hard, reflecting surface. These =

surfaces will reflect sound toward the rear of the room. In order to =
maintain a=20
low reverberation time with reflectors in the room, it will likely be =
necessary=20
to add absorptive materials on the side and rear walls. The need for =
reflectors=20
depends on the teaching methods used. For example, reflectors are useful =
in=20
rooms used mostly for lecturing, but are not needed in rooms used only =
for=20
small-group work or as laboratories.=20
<P>
<CENTER><IMG =
src=3D"http://asa.aip.org/classroom/reverberation.jpg"></CENTER>
<P>
<H3>MECHANICAL EQUIPMENT NOISE</H3>
<P>High ambient noise from mechanical equipment such as noisy heating,=20
ventilation and air conditioning (HVAC) systems is all too common in =
existing=20
schools. This is a serious problem for teachers and students alike. =
Teachers=20
must raise their voices to maintain the +10 dB signal-to-noise ratio =
necessary=20
for good speech intelligibility. That results in many teachers taking =
several=20
sick days each year as a result of vocal strain, costing taxpayers money =
that=20
would have been better spent on quiet mechanical equipment. At the same =
time,=20
students must either struggle to hear or else become distracted and stop =
paying=20
attention. Mechanical noise is primarily the result of poor planning and =
can be=20
difficult and expensive to fix in existing classrooms. However, =
excessive=20
mechanical noise can be eliminated at little or no extra cost if the =
system is=20
designed properly in the first place. Mechanical engineers are sometimes =
unaware=20
of or insensitive to this problem, and should be reminded that noise =
control is=20
a critical issue that must be handled during the design and purchasing =
process.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/problems.jpg"></CENTER>
<P>There are many methods for measuring the loudness of mechanical =
noise. A good=20
guideline is that the noise level in classrooms should not exceed NC 25 =
to 30.=20
The NC, or Noise Criteria, rating is determined by measuring noise =
levels at=20
certain frequencies, plotting these levels on a graph, then comparing =
the=20
results to established NC curves. (A more detailed explanation is =
contained in=20
the Appendix.) Another useful guideline is that the noise level should =
not=20
exceed 35 dBA. This is an easily measured, single-number rating of the =
noise=20
level over all frequencies that reduces the indicated noise level at =
lower=20
frequencies to simulate the sensitivity of the ear. Typically, the noise =
level=20
of a room in dBA is 5 to 7 dB higher than the NC rating. (Converting =
sound=20
levels as measured in octave frequency bands to dBA is also explained in =
the=20
Appendix.)=20
<P>Finding the source of mechanical noise in a room is sometimes as =
difficult as=20
finding the proverbial needle in a haystack. The noise can originate =
from one or=20
many sources, and complex cases are best handled by a professional =
acoustical=20
consultant with the skills and equipment to locate and reduce the levels =
of all=20
noise sources. Bearing that in mind, Figure 4 lists a few common =
problems you=20
can look for in an existing classroom with excess mechanical noise =
resulting=20
from a central mechanical system that distributes air to the rooms =
through=20
ductwork.=20
<P>For mechanical system noise the old adage, =93an ounce of prevention =
is worth a=20
pound of cure,=94 is certainly true. To limit such noise, keep the =
following=20
guidelines in mind when designing new classrooms:=20
<P>
<OL>
  <LI>Locate rooftop mechanical equipment, VAV boxes, and fan-coil units =
away=20
  from critical listening spaces such as classrooms. Positioning units =
over=20
  hallways and running ducts to nearby classrooms is one good solution. =
Avoid=20
  placing any major mechanical equipment inside, above, below, or =
adjacent to=20
  classrooms.=20
  <LI>Select air handlers with low sound-level ratings.=20
  <LI>Size ducts large enough to permit low air velocities. Select =
diffusers=20
  with NC ratings below 20 to 25.=20
  <LI>Spend a little extra on longer duct runs. This pays dividends in =
reduced=20
  mechanical noise and crosstalk (the transmission of sound between =
rooms via=20
  ductwork). See Figure 5 for an example of good and bad duct =
arrangement.=20
  <P>
  <CENTER><IMG src=3D"http://asa.aip.org/classroom/ducts.jpg"></CENTER>
  <LI>Avoid using unit ventilators, fan coil units and ductless split =
systems in=20
  classrooms. These units contain fans and sometimes compressors that =
are=20
  notoriously loud and difficult to treat due to their position in the=20
  classroom.</LI></OL>
<P>
<H3>INTERIOR NOISE SOURCES</H3>
<P>Noise from adjacent rooms disrupts the learning process, especially =
during=20
quiet reading times or test-taking. Fifty years ago, when school walls =
were=20
typically built of heavy brick or concrete block, this was not as much =
of a=20
problem. In recent decades, the need to lower construction costs has led =
to the=20
use of thin, lightweight wall materials that provide little noise =
reduction.=20
Even worse, in the 1960s and 1970s many open plan classrooms were built =
with no=20
partitions whatsoever between classrooms. In some schools, such spaces =
have=20
since been partitioned, but noise reduction between rooms may still be=20
insufficient.=20
<P>If you are unsure whether the wall between two existing classrooms is =

adequate, try this simple test: Set up a television or video monitor in =
one room=20
and set the sound level so it can be comfortably heard in the back of =
the=20
classroom. Then go into the neighboring classroom and listen for sounds =
from the=20
equipment next door. If sounds are faint or inaudible, the barrier is=20
sufficient. If sounds are fairly loud, and especially if words are =
intelligible,=20
the partition between the rooms needs to be improved.=20
<P>Figure 6 shows examples of both good and bad gypsum board wall =
construction.=20
In general, as the mass of a wall is increased, its noise reduction also =

increases. However, a thick, solid wall is usually too expensive and =
heavy and=20
wastes valuable floor space. Therefore, an effective compromise is to =
construct=20
a wall of a layer of heavy material, an airspace, and another layer of =
heavy=20
material. A typical example would be a stud wall having two layers of =
5/8 inch=20
thick gypsum board on each side. When constructing such a wall, be sure =
to=20
overlap the layers of gypsum board so the joints on both layers do not =
line up=20
and create a gap that sound can pass through. Adding glass fiber or =
mineral=20
fiber insulation to the cavity in the middle of the wall can also reduce =
noise=20
transmission.=20
<P>In terms of noise reduction, a wall is like a chain: it is only as =
strong as=20
its weakest link.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/gypsum.jpg">=20
<P><IMG src=3D"http://asa.aip.org/classroom/doors.jpg"></CENTER>
<P>Windows, doors, small gaps, cracks, grilles, louvers, etc. can =
completely=20
negate a wall=92s effectiveness. Gaps between walls and the floor and =
ceiling=20
should be sealed with an acoustical sealant. Thin or hollow-core doors =
with=20
large gaps under them commonly cause sound leaks in otherwise good =
walls. Solid=20
doors with tight-fitting, sealed frames are best. Their location also =
matters.=20
For example, it is best not to pair up doors to adjacent rooms, as this =
provides=20
a short path through which sound may travel from one room, through the =
doors,=20
and into the next room. (Figure 7 shows both good and bad layouts.) =
Also,=20
classroom doors should not be placed directly across a hall from one =
another.=20
Staggering doors across a hallway creates a longer, less direct path for =
noise=20
to travel from one room to another.=20
<P>To be effective, partition walls should extend from the structural =
floor to=20
the structural ceiling. Otherwise, sound from one room can easily pass =
through a=20
lay-in acoustical tile ceiling, over the partition wall, and down =
through the=20
lay-in ceiling of the next room. (See Figure 8.) This is commonly =
overlooked=20
when walls are added during renovations, such as when open-plan =
classrooms are=20
partitioned.=20
<P>Preventive design can often eliminate the need for thick, expensive =
walls.=20
During the design process, consider which rooms will be noisy =
(mechanical rooms,=20
gymnasiums, cafeterias, music rooms, industrial design shops, etc.) and =
use=20
buffer areas (hallways, storage rooms, and restrooms) to separate these =
spaces=20
from critical listening areas (classrooms, libraries, special education =
areas,=20
and offices).=20
<P>
<H3>EXTERIOR NOISE SOURCES</H3>
<P>The noise reduction of exterior walls is also important since many =
noisy and=20
potentially disruptive activities go on outside the school. Most schools =
are=20
built with brick or concrete block exterior walls, which are good sound=20
barriers, but with inadequate windows that permit considerable sound=20
transmission. To provide noise reduction, windows must be well sealed.=20
Double-paned glass provides better noise reduction than single-paned =
glass (as=20
well as better thermal insulation and decreased energy costs). Other =
common=20
sound leakage culprits are wall-mounted unit ventilators that duct =
directly=20
outside. These units not only transmit exterior noise but generate ample =
noise=20
themselves; they should be avoided whenever possible.=20
<P>During site planning, consider external noise sources that could =
disrupt=20
learning and attempt to locate classrooms away from such areas. Common =
noise=20
sources include: aircraft flyovers, busy roads, idling school buses,=20
playgrounds, playing fields, exterior mechanical equipment, dumpsters =
being=20
emptied by garbage trucks, lawn mowers, and noisy machinery in nearby =
buildings.=20

<P>
<H3>SOUND REINFORCEMENT</H3>
<P>Sound reinforcement systems, often referred to as =93soundfield=94 or =
=93soundfield=20
FM=94 systems, are sometimes suggested as relatively inexpensive =
solutions for=20
classrooms with poor signal-to-noise ratios.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/travels.jpg">=20
<P><IMG src=3D"http://asa.aip.org/classroom/open.jpg"></CENTER>
<P>A typical system consists of a wireless microphone worn by the =
teacher and=20
one or more loudspeakers located at the front of the room, in the =
ceiling, or=20
along the walls to distribute the sound to the students. Amplifying the=20
teacher=92s voice raises the signal-to-noise ratio, which improves =
speech=20
intelligibility and reduces vocal strain. This can be useful in a room =
with a=20
moderate amount of mechanical noise that would otherwise be difficult or =

expensive to silence. However, such systems also have their limitations. =
An=20
overly-reverberant classroom, for example, will cause the sound from the =

loudspeakers to build up and remain unintelligible. Whether or not a =
sound=20
reinforcement system is used in the classroom, it is vital to employ =
acoustical=20
treatments that reduce reverberation time.=20
<P>Another drawback to sound reinforcement systems is that they amplify =
only the=20
teacher. Students are not amplified when they ask the teacher questions =
or talk=20
among themselves while working in groups. Some systems provide an extra =
handheld=20
microphone that students can pass around. However, this is a cumbersome =
solution=20
that interferes with spontaneous discussions. Also, if the microphone is =
not=20
kept close to the person speaking, it will pick up as much ambient noise =
as=20
speech, and the S/N will not be improved. Still another problem is that =
the=20
amplified sound will become noise for adjacent classrooms. Despite these =

shortcomings, sound reinforcement systems can be cost-effective =
improvements for=20
classrooms with high noise levels, and are usually better than no =
modifications=20
at all.=20
<P>
<H3>EXAMPLES OF GOOD AND BAD CLASSROOMS</H3>
<P>How do all of these pieces of the puzzle fit together? This section =
provides=20
examples of good and bad classroom acoustics to illustrate how =
architectural=20
finishes can be used to control reverberation and echoes.=20
<P>From an acoustical standpoint, open-plan classrooms are perhaps the =
worst.=20
While they can be advantageous for certain teaching methods or student=20
interaction, they have serious acoustical drawbacks. Students are easily =

distracted by acoustical and visual signals that spill over from =
adjacent=20
classes. And if students with hearing impairment or attention deficit =
disorders=20
have difficulty concentrating on the teacher=92s voice in a classroom =
with loud=20
mechanical noise, consider their plight in a classroom where the =
background=20
noise is not random but rather an intelligible signal. To combat these =
problems,=20
many open-plan classrooms have been divided with partial-height =
partitions or=20
operable partitions that slide out like curtains. While these barriers =
do help=20
students focus by eliminating visual distractions, they provide little =
noise=20
reduction between classrooms. (Figure 9 shows an example of an open =
plan.)=20
<P>Another undesirable design is the classroom with a tall plaster or =
gypsum=20
board (hard) ceiling, hard walls and hard tile floor. In such a =
classroom,=20
echoes and reverberation tend to destroy speech intelligibility, =
especially for=20
young children. Unlike mechanical noise, reverberation cannot be =
overcome by=20
raising the level of the teacher=92s voice. An acoustical treatment must =
be added=20
to increase absorption and reduce harmful echoes. (See Figure 10a.) For=20
suggestions on materials, refer to the section in the Appendix on =
reverberation=20
time. For a nontraditional solution, read the case study below.=20
<P>Simply including a sound-absorbing lay-in ceiling and thin carpet on =
the=20
floor will usually result in good classroom acoustics and low =
reverberation=20
time. This solution is inexpensive for new construction and is also an=20
affordable way to renovate existing classrooms. For small to =
moderate-sized=20
classrooms, the lay-in ceiling will provide an acceptable reverberation =
time,=20
provided that acoustical ceiling tiles with an NRC greater than 0.75 are =
used.=20
The carpet adds some high-frequency absorption, but primarily serves to =
reduce=20
self-noise from the students. (Refer to Figure 10b.) Unfortunately, this =

approach does nothing to control echoes from the walls. However, =
thoughtful=20
arrangement of furniture such as cabinets and bookcases can help break =
up large,=20
flat walls and reduce echoes.=20
<P>The best design for a lecture-style classroom would be to move some =
of the=20
absorption from the ceiling to the walls and keep the middle of the =
ceiling hard=20
to reflect the teacher=92s voice toward the back of the room. This =
seemingly=20
complex, partially absorptive and partially reflective ceiling can be =
easily=20
built with a standard ceiling grid. Simply place acoustical ceiling =
tiles around=20
the perimeter of the ceiling and gypsum board panels in the center of =
the grid.=20
To reflect more sound to the back of the room, the ceiling can be shaped =
over=20
the teacher=92s location at the front of the room. This reflecting =
surface should=20
be built from a hard material like plywood or gypsum board, and can be =
painted=20
to match the room. Placing absorptive materials on the walls =
simultaneously=20
reduces reverberation time and kills echoes. Fabric-covered, 2 inch =
thick glass=20
fiber panels are a good choice because they are attractive, fairly =
rugged, and=20
provide some absorption at low frequencies. Add thin carpeting to the =
floors,=20
and the result can be an acoustically wonderful classroom, with a low=20
reverberation time, no echoes, proper distribution of reflections, and =
low=20
self-noise, all achieved with common building materials. (See Figure =
10c.)=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/layouts.jpg"></CENTER>
<P>
<H3>CASE STUDY -OLDER CLASSROOM</H3>
<P>The topic of this case study is a classroom in an older university =
building=20
that was the subject of complaints from teachers about the generally =
poor=20
acoustical conditions including high noise levels and poor speech=20
intelligibility. While this is a university classroom, its design is =
typical of=20
many classrooms in older elementary and secondary schools. The room, =
shown in=20
Figure 11, has high plaster ceilings and many tall windows. The building =
was=20
originally constructed with no central air conditioning system, so =
several=20
window air conditioners were added, which were very noisy. In order to =
properly=20
prepare recommendations for improving the acoustical conditions of this =
room,=20
the ambient noise levels as established by the window air conditioning =
units=20
were measured and the reverberation times of the room were also =
measured. It was=20
important that acoustical conditions be improved without adveresly =
affecting=20
room aesthetics.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/older.jpg"></CENTER>
<P>Due to the high ceiling and lack of absorptive materials in the room, =

reverberation time was an unsatisfactorily long 1.5 seconds at middle=20
frequencies. Adding a suspended ceiling of acoustical ceiling tiles =
would have=20
improved the space acoustically but not visually. To avoid interfering =
with the=20
tall windows, the suspended ceiling would have to be sloped up at the =
sides, and=20
a new lay-in ceiling would not have matched the traditional architecture =
of the=20
classroom. Instead, 2 inch thick, dense glass fiber panels, covered with =
fabric=20
that complemented the color scheme in the room, were suspended from the =
ceiling=20
at the same level as the existing pendant-mounted lighting fixtures. =
This=20
resulted is an aesthetically pleasing solution without the expense of =
replacing=20
the lighting fixtures, which would normally be necessary when adding a =
suspended=20
ceiling. Fabric faced glass fiber panels were also mounted on the walls =
between=20
the windows to prevent echoes and further decrease reverberation time. =
After=20
modification, the unoccupied reverberation time was reduced to a =
desirable 0.5=20
seconds in the middle frequencies. Similar solutions could be applied to =
many=20
classrooms where suspended acoustical tile ceilings are not suitable.=20
<P>The air conditioning system for this room was also modified with =
mixed=20
acoustical results. The original window air conditioners created an =
unacceptably=20
high noise level described by NC-57. The school decided to replace the =
window=20
units with a wall mounted, two speed fan/coil unit and with the =
compressor=20
properly located outside. This improved room cooling but it did not =
completely=20
solve the noise problem. With the fan at high speed, the noise in nearby =
seating=20
areas is NC-47, 10 points lower than the original NC-57, but still not =
suitable.=20
On the opposite side of the room the noise is NC-43. with the fan at low =
speed=20
the noise is NC-36 and NC-33. With low speed operation the noise is =
relatively=20
close to the criteria (see page 4). But, at high speed the noise is=20
significantly above the criteria. When in-room fan/coil units must be =
used for=20
economic or physical reasons, multi-speed units should be employed, and =
the=20
units should be capable of handling the cooling task with low speed fan=20
operation.=20
<P>
<H3>ACOUSTICAL GUIDELINES FOR SPECIAL ROOMS</H3>
<P>Though this booklet is primarily intended to provide guidelines on =
classroom=20
acoustics, this section addresses acoustical issues for other common=20
schoolrooms. While these guidelines are not as comprehensive as the =
material on=20
classrooms, much of the material presented earlier, such as the need to=20
eliminate mechanical noise and provide effective noise reduction, also =
applies=20
to rooms such as cafeterias, gymnasiums, and auditoriums. This section =
does not=20
attempt to cover music education rooms since the acoustics of these =
spaces are=20
especially critical. Special purpose rooms are complex and best handled =
by a=20
professional acoustical consultant.=20
<P>The most common problem plaguing cafeterias and gymnasiums is =
excessive=20
reverberation time (RT), since they typically have both large physical =
volume=20
and hard surface materials. In cafeterias, this long RT causes noise =
buildup,=20
with students having to speak louder and louder to hear each other until =
there=20
is a continuous roar. In gymnasiums, which are frequently used for pep =
rallies=20
and assemblies, combining poor acoustics with a badly designed sound =
system=20
produces speech that is nearly unintelligible and wreaks havoc on music. =

<P>Several options are available for improving sound absorption in these =
large=20
spaces. In new construction, if the ceiling is constructed as an exposed =
metal=20
deck, consider using metal deck with perforations on the bottom and =
glass fiber=20
above to absorb sound. This will significantly reduce reverberation time =
without=20
adding unduly to construction costs. Another option for either new =
construction=20
or renovation is to hang absorptive baffles or banners from the ceiling. =
Baffles=20
and banners are commercially available products made of several inches =
of glass=20
fiber covered with thin plastic or cloth. They are easily installed, =
available=20
in a rainbow of colors, and do not detract from the appearance of the =
room.=20
Placing glass fiber or wood fiber panels on the walls will also reduce =
both RT=20
and echoes.=20
<P>Gymnasiums and cafeterias tend to be noisy spaces, and this noise can =
also=20
disrupt nearby classrooms. Thus, separate these areas from classrooms, =
and do=20
not place classrooms beneath gymnasiums. The impact noise from bouncing=20
basketballs and the like is a severe problem that is expensive to =
correct in new=20
construction and even more expensive in renovations.=20
<P>School auditoriums accommodate a variety of activities, including =
speech,=20
theater, dance, and music. All these activities require good acoustics, =
but each=20
has different acoustical requirements. To meet the needs of all these=20
activities, an auditorium=92s acoustics must either be compromised so it =
performs=20
adequately for all functions, but favorably for none, or else a =
technique called=20
=93variable acoustics=94 must be used to adapt its acoustics to suit =
each function.=20
Variable acoustics involves the use of panels, drapery, and other =
materials that=20
can be easily rearranged to alter reflections, reverberation time, and =
other=20
acoustical properties. To achieve satisfactory results for these complex =
rooms ,=20
it is best to seek the assistance of a professional acoustical =
consultant. That=20
said, the following paragraphs provide a few design guidelines to follow =
and=20
common pitfalls to avoid.=20
<P>Combining the auditorium with the cafeteria or gymnasium is a =
tempting way to=20
save both money and square footage. Unfortunately, this rarely, if ever, =
results=20
in an acoustically satisfactory auditorium since the rooms have =
conflicting=20
requirements. In an auditorium, the objective is to reinforce sound from =
a=20
single location, while in cafeterias and gymnasiums the goal is to =
suppress=20
noise from many sources. This conflict cannot be resolved effectively, =
so these=20
room combinations should be avoided. In an auditorium, the shape of the =
room is=20
important to properly reflect sound into the audience. Avoid wide, =
fan-shaped=20
halls with concave rear walls having a radius centered on the stage. A =
concave=20
rear wall will focus disturbing echoes back to the performers on stage, =
and if=20
the side walls are splayed too wide, they will not provide useful early=20
reflections into the seating. To allow reflected sound to reach those =
seated in=20
the back, under balcony depth should be less than twice the distance to =
the=20
floor below. A flat ceiling will send all reflections to the back of the =
hall,=20
so sections of the ceiling should be angled to spread reflections =
throughout the=20
audience. Convex diffusing panels shaped like pyramids or cylinders or =
special=20
=93QRD=94 diffusers help scatter sound throughout the auditorium and =
reduce discrete=20
echoes. Walls can be covered with heavy drapery that slides horizontally =
or=20
rises vertically to add absorption when necessary and remove it when=20
unnecessary.=20
<P><B>NOTE</B>: An ANSI Standard on classroom acoustics is presently =
under=20
development. Contact the Acoustical Society of America for further =
information.=20
(See the back cover for the address, phone number and website.)=20
<P>
<HR>

<P>
<H2>APPENDIX</H2>
<P>
<H3>FREQUENCY</H3>
<P>Frequency is an important factor in most acoustical measurements. =
Sound=20
occurs when a vibrating source causes small fluctuations in the air, and =

frequency is the rate of repetition of these vibrations. Frequency is =
measured=20
in hertz (Hz), where 1 Hz =3D 1 cycle per second. A young person with =
normal=20
hearing can detect a wide range of frequencies from about 20 to 20,000 =
Hz. In=20
order to deal with such a large spectrum, acousticians commonly divide =
the=20
frequency range into sections called <B>octave bands</B>. Each octave =
band is=20
identified by its center frequency. For the standard octave bands these =
center=20
frequencies are: 63, 125, 250, 500, 1000, 2000, 4000, and 8000 Hz. As =
you can=20
see, the ratio of successive frequencies is 2:1, just like an octave in =
music.=20
This also correlates with the sensitivity of the ear to frequency, since =
a=20
change in frequency is more readily distinguished at lower frequencies =
than at=20
higher ones. For example, the shift from 100 to 105 Hz is more =
noticeable than=20
the shift from 8000 to 8005 Hz. Higher-frequency octave bands contain a =
wider=20
range of frequencies than lower-frequency octave bands, but we perceive =
them as=20
approximately equal. To obtain a more detailed indicator of the spectrum =
of=20
sound power, measurements are often made in the one-third octave =
frequency=20
bands. Standard center frequencies for the one-third octave bands are: =
50, 63,=20
80, 100, 125, 160, 200, 250, 315, 400, 500, 630, 800, 1000 Hz, etc. Note =
that an=20
octave band contains the one-third octave band at the standard octave =
band=20
center frequency plus the one-third octave bands on each side.=20
<P>
<H3>DECIBELS</H3>
<P>The most common measure of a sound=92s level is Sound Pressure Level, =
or SPL,=20
expressed in decibels, abbreviated dB. Decibels are not typical units =
like=20
inches or pounds in that they do not linearly relate to a specific =
quantity.=20
Instead, decibels are based on the logarithmic ratio of the sound power =
or=20
intensity to a reference power or intensity. Sound power and intensity =
are not=20
easy to measure. However, sound pressure is easily measured with a sound =
level=20
meter. Sound pressure may also be expressed in dB since sound pressure =
squared=20
is proportional to sound power or intensity. We use dB instead of the =
actual=20
amplitude of the sound in units of pressure because its logarithmic =
value=20
represents the way our ears interpret sound and because the numbers are =
more=20
manageable for our calculations. Most sounds fall in the range of 0 =
to140 dB,=20
which is equivalent to waves with pressures of 20 to 200,000,000 =
micropascals=20
(or 2 x 10 -10 to 2 x 10 -2 atm). To help you get a feeling for sound =
pressure=20
levels (in dB), the approximate SPLs of some common sound sources are =
given in=20
Figure 12.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/pressure.jpg"></CENTER>
<P>A simple sound level meter combines sound pressure levels over all=20
frequencies to give the overall SPL in dB. More complex meters have =
filters that=20
can measure the SPL in each octave band or one-third octave band =
separately so=20
we can identify the level in each band, thus identifying the spectrum of =
the=20
sound. Sound level meters can also =93weight=94 the sound pressure level =
by=20
adjusting the level in different frequencies before combining the levels =
into a=20
weighted overall level. For example, A-weighting reduces the level of =
sounds at=20
low frequencies to simulate the variations in sensitivity of the ear to=20
different frequencies. A-weighted values are denoted as dBA to =
differentiate=20
them from unweighted dB levels. Similarly, C-weighted values are labeled =
dBC.=20
C-weighting slightly reduces the level of sounds below 50 and above 5000 =
Hz, but=20
is nearly flat in between, and can be used to approximate an unweighted =
reading=20
on sound level meters that only offer A- or C-weighting. Comparing A- =
and=20
C-weighted levels for a noise source can provide a rough estimate of its =

frequency distribution. If the two levels are within 1 or 2 dB, most of =
the=20
noise is above 500 Hz. If the two levels vary by more than a few dB, a=20
significant amount of the noise is in the lower frequencies. To convert=20
unweighted octave band sound pressure levels into weighted A or C =
levels, add or=20
subtract the amounts noted in Figure 13 from the corresponding frequency =
bands.=20
Next, sum the octave band levels (two at a time as explained below) to =
arrive at=20
the overall dBA or dBC value.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/dbscales.jpg"></CENTER>
<P>As mentioned earlier in the text, calculating the SPL of two sources =
together=20
is not as simple as adding their individual decibel levels. Two people =
speaking=20
at 70 dBA each are not as loud as a jet engine at 140 dBA. To combine =
two=20
decibel values, they must be converted back to pressure squared, summed, =
and=20
converted back to decibels. The mathematics may be approximated by using =
Figure=20
14.=20
<P>
<CENTER><IMG =
src=3D"http://asa.aip.org/classroom/addition.jpg"></CENTER>If one=20
sound is much louder than the other, the louder sound drowns out the =
softer=20
sound, and the combined decibel level is just the level of the louder =
sound. If=20
the two sounds are equally loud, then the combined level is 3 dB higher. =
More=20
than two sources can be combined, but they must be considered two at a =
time. For=20
example, an unbuilt classroom is expected to have 34 dBA of mechanical =
system=20
noise, a computer that generates 32 dBA of noise, and an overhead =
projector that=20
generates 43 dBA. What will be the total sound pressure level from the =
three=20
noise sources? The difference between the first two decibel values is: =
34- 32=3D2,=20
so add 2 dB to the higher value: 34+2=3D36 dBA. Then combine this with =
the=20
projector noise: 43-36=3D7, so add 1 dB to the higher value: 43+1=3D 44 =
dBA total=20
from the three noise sources. If the SPL of the teacher=92s voice is 55 =
dBA, what=20
is the signal-to- noise ratio in the room? 55-44=3D +11 dB, which is =
sufficient=20
for good speech intelligibility. How much louder is the total 44 dBA =
than each=20
of the individual noise sources? Due to the response of our ears, we can =
just=20
notice a difference of 3 dB. An increase of 10 dB sounds approximately =
twice as=20
loud, and an increase of 20 dB sounds about four times as loud.=20
<P>
<H3>REVERBERATION TIME</H3>
<P>Over 100 years ago, a Harvard physics professor named Wallace Clement =
Sabine=20
developed the first equation for reverberation time, which has since =
been named=20
after him and is still used today. Reverberation time is defined as the =
length=20
of time required for sound to decay 60 dB from its initial level. =
Sabine=92s=20
simple formula is:=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/formula.jpg"></CENTER>
<P>where:=20
<P>
<BLOCKQUOTE>RT(60) =3D reverberation time (sec)<BR>V =3D room volume=20
  (ft<SUP>3</SUP> )<BR>S =3D surface area (ft <SUP>2</SUP> )<BR>? =3D =
absorption=20
  coefficient of material(s) at given frequency<BR>? indicates the =
summation of=20
  S times ? for all room surfaces</BLOCKQUOTE>
<P>To use this formula, the volume of the room, surface area of each =
material in=20
the room, and absorption coefficients for those materials must be known. =

Absorption coefficients are measured in specialized laboratories, and =
represent=20
the fraction of sound energy (not sound level-dB) the material will =
absorb as a=20
decimal from 0 to 1. Figure 15 gives absorption coefficients for common=20
classroom materials.=20
<P>A commonly used one-number rating called <B>NRC, Noise Reduction=20
Coefficient</B>, is simply the average of the absorption coefficients at =
250,=20
500, 1000, and 2000 Hz. This simple, one-number rating can be useful for =

comparing the relative absorption of two materials; however, examining=20
absorption coefficients in each octave band gives a better idea of the=20
performance of a material at various frequencies.=20
<P>Reverberation time is often calculated with the room unoccupied. =
Since people=20
and their clothing provide additional sound absorption, an unoccupied =
room is=20
the worst-case scenario, though not an unreasonable one, since occupancy =
of most=20
classrooms varies. In a complete analysis, this calculation should be =
performed=20
for each octave band, as the RT can vary widely at different =
frequencies.=20
However, for a quick estimate, the RT of a classroom can be calculated =
for just=20
one octave band representative of speech frequencies, such as 1000 Hz. =
If this=20
RT is acceptable, then the RT throughout the speech range will likely be =

acceptable.=20
<P>To demonstrate the use of the Sabine equation, Figure 16 provides an =
example=20
calculation of the RT at 500 Hz for the acoustically poor classroom =
example=20
given in Figure 10a. Try calculating the RT at 500 Hz of the =
acoustically=20
satisfactory classroom in Figure 10b with only a sound-absorbing ceiling =
added.=20
Note that the ceiling is lower in that example, so the volume and =
surface areas=20
will change. The RT of the satisfactory classroom is approximately 0.4 =
seconds.=20
<P>
<CENTER><IMG =
src=3D"http://asa.aip.org/classroom/calculation1.jpg"><BR><IMG=20
src=3D"http://asa.aip.org/classroom/calculation2.jpg"></CENTER>
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/levels.jpg"></CENTER>
<P>
<H3>SPEECH INTELLIGIBILITY</H3>
<P>There are many methods for measuring or predicting speech =
intelligibility,=20
ranging from a simple A-weighted sound level to the complex <B>Speech=20
Transmission Index (STI)</B>. For classrooms, speech intelligibility can =
be=20
predicted from reverberation time and signal-to- noise ratio. A =
classroom with a=20
0.5 second RT and +10 dB S/N will have approximately 90 percent speech=20
intelligibility. If the RT is kept at 0.5 seconds but the S/N is reduced =
to 0=20
dB, intelligibility falls to about 55 percent. Similarly, if the S/N is =
+10 dB=20
but RT is increased to 1.5 seconds, intelligibility drops to around 75 =
percent.=20
And if the S/N falls to 0 dB and RT is 1.5 seconds, intelligibility =
falls=20
dramatically to approximately 30 percent. Sadly, this last condition =
does exist=20
in some U.S. classrooms.=20
<P>Speech intelligibility tests can be used to measure intelligibility =
in=20
existing classrooms. Such tests can take many forms. Typically, a =
speaker reads=20
nonsense syllables, monosyllabic words, or sentences, and listeners =
record what=20
they hear, or choose from a list of possible alternatives. The =
percentage of=20
test items correctly heard is a measure of speech intelligibility. =
Standardized=20
tests have been developed that outline test procedure, selection of =
listeners,=20
training of speakers and listeners, and so on. Also available are =
recordings of=20
standardized word lists that can be reproduced instead of having a =
speaker read=20
from a list. This eliminates lip reading cues and variations in =
different=20
speakers=92 speech characteristics and speech levels. Before beginning =
actual=20
testing, listeners should practice taking the tests in a quiet =
environment until=20
they are familiar with the procedure and their scores reach a stable =
level.=20
(Words used are randomly chosen from a standardized list so listeners =
cannot=20
simply memorize the order of the words.)=20
<P>When testing in a classroom, the speaker should read the list from =
the=20
teacher=92s usual speaking location. To assure conservative results, =
several=20
listeners should be seated together in whichever area of the classroom =
has the=20
poorest signal-to-noise ratio. This is typically in the back, or near =
the=20
loudest source of mechanical noise. Any noises present during normal =
classroom=20
use, such as mechanical noise, outdoor noise, or corridor noise, should =
be=20
present to ensure representative values of speech intelligibility.=20
<P>Adults average roughly 10 percent better than young children on =
speech=20
intelligibility tests. For example, in a first-grade classroom in which =
adult=20
listeners score 90 percent, typical students will likely score only 80 =
percent.=20
Students with hearing or learning disabilities, or for whom English is a =
second=20
language, will show even lower scores. If speech intelligibility in a =
classroom=20
is less than 90 percent, acoustical treatments should be implemented to =
reduce=20
reverberation and/or improve signal-to-noise ratio.=20
<P><B>NOTE</B>: Speech intelligibility testing is not a simple procedure =
and=20
professional advice is suggested. The school audiologist may be a good =
resource=20
in this regard.=20
<P>
<H3>NOISE CRITERIA RATING</H3>
<P>The noise level in a space can be effectively described with a =
single-number=20
rating called the noise criteria (NC) rating. The NC rating is =
determined by=20
measuring the sound pressure level of the noise in each octave band, =
plotting=20
these levels on a graph, and then comparing the results to established =
NC=20
curves. The lowest NC curve not exceeded by the plotted noise spectrum =
is the NC=20
rating of the sound. On most graphs, NC curves are shown in intervals of =
5 to=20
save space, but the NC rating can be given as any whole number in =
between, not=20
just as a multiple of 5. To illustrate this, we will find the NC rating =
for the=20
window air conditioners, unit ventilator, and background noise from the =
case=20
study presented above. (See Figures 17 and 18.) A blank NC chart has =
been=20
provided. (See Figure 19.)=20
<P>
<H3>SOUND LEVEL VS. DISTANCE</H3>
<P>We all know that sound level decreases as the distance from a sound =
source=20
increases. This decrease in sound level is quantified by the inverse =
square law.=20
That is, the sound energy decrease is proportional to the square of the =
distance=20
increase. For example, if the listening distance from a sound source is=20
increased by a factor of 2 (doubled), the direct sound energy is =
decreased by a=20
factor of 4 or 2 squared (2 times 2). This translates to a 6 dB =
reduction in the=20
sound intensity level and the sound pressure level of the direct sound =
for each=20
doubling of the distance from the sound source.=20
<P>Let=92s assume that, in a particular classroom, the average =
difference between=20
the sound level of the teacher=92s voice and the level of the classroom =
background=20
noise produced by the air conditioning system is 10 dB at a student=92s =
listening=20
position 10 feet from the teacher. With this 10 dB signal-to-noise ratio =
the=20
intelligibility of the teacher=92s speech is probably satisfactory as =
discussed in=20
the previous section on speech intelligibility. But, if the distance =
from the=20
teacher to the student is doubled to 20 feet, the signal-to-noise ratio =
is=20
reduced to about 4 dB (assuming that the background noise remains =
constant). At=20
a distance of 30 feet the level of the direct sound produced by the =
teacher is=20
reduced by about 10 dB and the signal-to-noise ratio is 0 dB, with low =
speech=20
intelligibility. Thus, it is most important that the background noise =
level be=20
acceptable in all classroom locations if a proper S/N ratio is to be =
maintained=20
allowing satisfactory speech intelligibility.=20
<P>
<CENTER><IMG src=3D"http://asa.aip.org/classroom/curves.jpg">=20
<P><IMG src=3D"http://asa.aip.org/classroom/curves2.jpg"></CENTER>
<P>Visit the <A href=3D"http://www.ncac.com/">National Council of =
Acoustical=20
Consultants</A> for a list of professional acoustical consultants.=20
<P>To obtain additional copies, please contact:=20
<P>Acoustical Society of America<BR>Suite 1NO1<BR>2 Huntington=20
Quadrangle<BR>Melville, NY 11747<BR>Phone: 516.576.2360<BR>Fax:=20
516.576.2377<BR>Email: <A =
href=3D"mailto:asa@aip.org">asa@aip.org</A><BR><A=20
href=3D"http://asa.aip.org/">http://asa.aip.org/</A><BR>Copyright =A9 =
Acoustical=20
Society of America<BR>
<HR>
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