From: Subject: Classroom Acoustics Boooklet Date: Wed, 3 Dec 2003 16:54:08 -0000 MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_000_0000_01C3B9BE.1194E000"; type="text/html" X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2800.1165 This is a multi-part message in MIME format. ------=_NextPart_000_0000_01C3B9BE.1194E000 Content-Type: text/html; charset="Windows-1252" Content-Transfer-Encoding: quoted-printable Content-Location: http://asa.aip.org/classroom/booklet.html Classroom Acoustics Boooklet

Classroom Acoustics

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

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

This publication was printed in August, 2000.=20

INTRODUCTION

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

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

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

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

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

THE BASICS

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

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: intensity and frequency. = 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

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: Transmission-- The sound passes through the = surface=20 into the space beyond it, like light passing through a window.=20 Absorption-- The surface absorbs the sound like a sponge absorbs = water.=20 Reflection-- The sound strikes the surface and changes direction = like a=20 ball bouncing off a wall. Diffusion-- 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

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 = Absorption=20 Coefficient ( a) and NRC (noise reduction coefficient) are = used to=20 specify the ability of a material to absorb sound.=20

A special problem that results from reflected sound is that of = discrete=20 echoes. 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

Another type of echo that interferes with hearing is flutter = echo.=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

Sound intensity levels and sound pressure levels can be measured in=20 decibels (dB). 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

An important acoustical measurement called Reverberation Time=20 (RT or RT(60)) 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

The Noise Reduction (NR) 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

Signal-to-Noise Ratio (S/N) 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

Speech intelligibility can be evaluated in existing rooms by = using=20 word lists. 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

For those interested in learning more about these topics, additional=20 information is provided in the Appendix.=20

ACOUSTICAL GUIDELINES FOR CLASSROOMS

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

REVERBERATION

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

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

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

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

UNDESIRABLE REFLECTIONS

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

USEFUL REFLECTIONS

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

MECHANICAL EQUIPMENT NOISE

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

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

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

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

  1. 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
  2. Select air handlers with low sound-level ratings.=20
  3. Size ducts large enough to permit low air velocities. Select = diffusers=20 with NC ratings below 20 to 25.=20
  4. 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

  5. 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.

INTERIOR NOISE SOURCES

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

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

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

In terms of noise reduction, a wall is like a chain: it is only as = strong as=20 its weakest link.=20

=20

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

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

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

EXTERIOR NOISE SOURCES

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

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

SOUND REINFORCEMENT

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

=20

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

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

EXAMPLES OF GOOD AND BAD CLASSROOMS

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

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

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

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

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

CASE STUDY -OLDER CLASSROOM

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

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

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

ACOUSTICAL GUIDELINES FOR SPECIAL ROOMS

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

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. =

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

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

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

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

NOTE: 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

APPENDIX

FREQUENCY

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 octave bands. 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

DECIBELS

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

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

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

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

REVERBERATION TIME

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

where:=20

RT(60) =3D reverberation time (sec)
V =3D room volume=20 (ft3 )
S =3D surface area (ft 2 )
? =3D = absorption=20 coefficient of material(s) at given frequency
? indicates the = summation of=20 S times ? for all room surfaces

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

A commonly used one-number rating called NRC, Noise Reduction=20 Coefficient, 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

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

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


SPEECH INTELLIGIBILITY

There are many methods for measuring or predicting speech = intelligibility,=20 ranging from a simple A-weighted sound level to the complex Speech=20 Transmission Index (STI). 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

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

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

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

NOTE: 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

NOISE CRITERIA RATING

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

SOUND LEVEL VS. DISTANCE

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

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

=20

Visit the National Council of = Acoustical=20 Consultants for a list of professional acoustical consultants.=20

To obtain additional copies, please contact:=20

Acoustical Society of America
Suite 1NO1
2 Huntington=20 Quadrangle
Melville, NY 11747
Phone: 516.576.2360
Fax:=20 516.576.2377
Email: asa@aip.org
http://asa.aip.org/
Copyright =A9 = Acoustical=20 Society of America

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