soundspace
Transcription
soundspace
PARAMETRIC STUDY OF SOUND PROPAGATION IN A CONCERT HALL SOUNDSPACE soundspace EPFL ENAC SAR ÉNONCÉ THÉORIQUE OSAMU MOSER LAUSANNE 11 01 2010 PARAMETRIC STUDY OF SOUND PROPAGATION IN A CONCERT HALL TABLE OF CONTENTS ii I. PREFACE XI i.i. Problematics xi i.ii. Field of interest xii i.iii. Methodology xiii 1. HISTORY OF SOUND SPACE 4 1.1. From Greeks to Modernity 4 1.2. Greek and Roman period (650BC - 400AD) 7 1.2.1. Theater and odea 7 1.2.2. Early acoustical knowledge 7 1.3. Early Christian period (400 - 800) 9 1.3.1. Church 9 1.3.2. Monody 9 1.4. Romanesque Period (800 - 1100) 10 1.4.1. Church 10 1.4.2. Organum 10 1.5. Gothic period (1100 - 1400) 11 1.5.1. Gothic cathedral 11 1.5.2. Plainchant, polyphony and miracle play 11 1.6. Renaissance (1400 - 1600) 13 1.6.1. Renaissance church and theater 13 iii iv 1.7. Baroque period (1600 - 1750) 15 1.7.1. Baroque church, theater and opera 15 1.7.2. Speech, Baroque and instrumental music 16 1.8. Classical period (1750 - 1825) 17 1.8.1. Concert hall and opera 17 1.8.2. Classical music 17 1.9. Romantic period (1825 - 1900) 19 1.9.1. Shoebox halls 19 1.9.2. Romantic music and acoustical knowledge 19 1.10. Modernity (1900 - today) 21 1.10.1. Concert halls and theaters 21 1.10.2. Modern acoustics 21 2. ACOUSTIC SPACE ANALYSIS 27 2.1. Selection samples 27 2.1.1. Concert halls and opera houses of the world 27 2.1.2. Selected concert halls and theaters 29 2.2. Type analysis 31 2.2.1. Comments for the type analysis diagram 34 2.3. Shape analysis 35 2.4. Seating arrangement 40 2.5. Section analysis 44 2.5.1. Section types 44 2.5.2. Comments for the section analysis diagram 44 2.6. Conclusion of the analysis 48 3. ARCHITECTURAL ACOUSTICS 53 3.1. Fundamentals of acoustics 53 3.1.1. Physical definition of sound 53 3.1.2. Representations of a single sound wave 54 3.1.3. Representation of multiple sound waves 54 3.1.4. Frequency 55 3.1.5. Absorption and reflection 55 3.1.6. Perception of sound 55 3.2. Measurable parameters 56 3.2.1. Reverberation time 56 3.2.2. Loudness 58 3.3. Number of seats 59 3.4. Further measurable parameters 60 3.4.1. Intimacy 60 3.4.2. Warmth 61 3.4.3. Envelopment 62 3.5. Conclusion on architectural acoustics 62 v vi 4. CONCERT HALL ENGINE 67 4.1. Introduction to the engine 67 4.2. The different applets of the engine 70 4.2.1. Volume 70 4.2.2. Stage area 70 4.2.3. Stage walls 70 4.2.4. Balcony section 71 4.2.5. Embracing walls 71 4.2.6. Seating area 71 4.3. Further extensions of the engine 72 4.3.1. Graphical input assistance 72 4.3.2. Lower seat dependence 72 5. PARAMETRIC CONCERT HALL 77 5.1. Site 77 5.2. Program 79 5.3. Design 81 5.3.1. Vineyard-style seating arrangement 81 5.3.2. Diamond form 81 APPENDIX : SCHEMES 85 REFERENCES 181 INDEX 187 vii preface i. PREFACE Being interested in parametric engines and organic architecture capable of responding to a series of constraints, I was looking for a topic where I can apply the know-how achieved in the two previous studio semesters. Thinking of space which needed mathematical computation in order to work properly, I was led to rooms for musical and visual spectacles and I started researching about the typology of concert halls and its underlying theory. It has to be said that this present booklet consists only in the presentation of a research that is still ongoing and is by no means a finalized product. Which is why the last chapters, for which I spent less time, are still quite short and represent more of a pool of ideas than effectively achieved work. i.i. Problematics Architectural acoustics can be described as something of a black art. Empiric studies led to knowledge we only recently started to understand in a scientific way. Perception of sound depends not only on the space, but also on the person listening to it. Digital sound propagation models (01): “L’architecture ne se fait pas sans l’acoustique. L’acoustique ne se fait pas sans architecture.” 1 1 Citation KAHLE, Eckhard, Kahle Acoustics, during a lecture at the EPFL, Switzerland, the 4th of November 2009. xi still need considerable computation power to give us more or less accurate results whether a hall offers a highly efficient acoustic distribution or not. Architects often tend to develop their projects on their own without consulting an expert such as an acoustician. Recent studies revealed a lot on architectural acoustics that give us rather precise information on how a spectacle space needs to be conceived to obtain certain characteristics. Translated in English, the citation in (01) expresses the fact that acoustics and architecture are depending on each other reciprocally, which underlines the necessity of starting to think about the acoustics from the first sketch on. i.ii. Field of interest Due to these stated concerns, I would like to create a tool that allows the architect to conceive a concert hall that responds to acoustical requirements from an engineering point of view, but still leaves him with as much conceptual freedom as possible. After directing some effort into computation of sound field performance and wave propagation inside a large room, I had to realize that this field of research needs far more work than I would be able to accomplish within the given time frame. Yoichi Ando for example has devoted several years of his professional career to create a so called “individual seat preference system”, based on subjective opinions of thousands of test persons that xii Preface had to rank sound they perceived in a seat that received a certain mix of sound.1 Finally I have chosen to conduct my research towards geometry and materiality of concert halls. I am looking for general forms, the dimensions, proportions and shape of a space, but also the constellation of balconies, distribution and seating areas and where which type of material is needed to achieve best performance. i.iii. Methodology The structure of this work represents also the methodology of my research, which was quite straight forward until present and consists in always finding a conclusion or synthesis before going to the next step. I tried hard to follow the recommendation of my guiding professor and assistant to merge the process of research and project design together. Unfortunately I could only do this partially, which is quite well visualized in the weighting of the different chapters. Concerning the structuring of this book, the first chapter treats the historical background (see chapter 1) of acoustic space, by comparing underlying theories and purposes of spectacle spaces during history. Secondly, I analyzed the different geometries of those acoustical spaces (see chapter 2) that allowed myself to get a grasp of different existing shapes of functioning concert halls. 1 ANDO, Yoichi, Architectural Acoustics - Blending Sound Sources, Sound Fields and Listeners, USA, Springers-Verlag New York Inc., 1998. xiii The next step consisted in retrieving technical background of sound propagation and concert hall acoustics. I did so by researching different parameters that result in good acoustics which are described in chapter 3. In the next chapter I am presenting the current state of my personal engine (see chapter 4), developed during the research, which should allow an architect to design a concert hall that offers good acoustic qualities without needing outstanding knowledge of architectural acoustics. The last part (see chapter 5) shows some ideas concerning the architectural project I would like to conduct for my master thesis. xiv Preface xv history CHAPTER 01 1. HISTORY OF SOUND SPACE Music and architecture, they both were born when human being started to try living more comfortable than other animals. Primitive songs around a camp fire and rudimentary coverage were the first precedents for arts that are now deeply rooted in human culture.1 1.1. From Greeks to Modernity In greek and roman antiquity already, architecture and music were quite close to each other. The proportion model used for architecture mainly during the Renaissance bears completely on the musical harmonic model. As a matter of fact, architects, musicians and philosophers consistently searched to create connections and to stimulate those two kind of arts. One of the most famous examples may be the citation by Philosopher Friedrich Schelling (02), which shows in a beautiful way how the relation of those two terms were perceived. Even though this quotation may seem (02): ”Architecture is frozen music.” 1 1 1 PASCHA, Khaled Saleh, Gefrorene Musik, Berlin, Dissertation for a Doctor in Engeneering, 2004, page 37. LONG, Marshall, Architectural Acoustics, USA, Elsevier Academic Press, 2006, page 1. 4 timeless, the relationship of architecture and music went through some change over time as I will try to explain with the next few paragraphs. Since the beginning of music, its expression was strongly dependant on the surrounding space that the local environment offered. By comparing for example African music and dance with early European music, we can easily note that the Africans developed a highly complex rhythmic character whilst Europeans stayed with a more melodic line. Wallace Clement Sabine (1868 - 1919), an early pioneer in architectural acoustics, felt that these two distinct developments could be due to the differences in their living environment. A possible explanation of the stated example would be that wooden huts and the open space in which African music is performed offered less reverberation and hence it needed to provide the rhythmic and tonal variety on its own. On the other hand, early European music was typically performed within highly reverberant enclosed space such as temples and churches, which did necessitate a complex tonal scale since reflections helped to give the music more depth. Gregorian chant is one of the styles that grew out of the acoustical characteristics specific to Gothic cathedrals.1 2 During the baroque period, in particular, composers were strongly dependant on the space in which their compositions were played. Before 1900, a concert was typically enacted only once, not several times as is the case today. In those days it was more important that the piece was in 1 2 5 Ibidem. FORSYTH, Michael, Architecture et musique, Belgium, Pierre Mardaga, 1985, page 29ff. Chapter 1: History Of Sound Space perfect harmony with the acoustical properties of the given hall. That is why composers wrote music with the specific acoustical characteristics of the space in mind in which their music was supposed to be performed.1 Today we can perceive another movement that has taken place within the relationship of music and architecture: since the greatest compositions of all time already exist, it is in the hand of architecture to adapt itself such as the performed music sounds as it is expected.2 In order to understand the development of the relation between music (03): “Before 1900, it was the music that had to adapt to the space. Today, it is the space that has to adapt to the music.” 1 1 Citation KAHLE, Eckhard, Kahle Acoustics, during a lecture at the EPFL, Switzerland, the 4th of november 2009. and architecture, I tried to investigate typical acoustic space, the underlying environment and music types at given periods of time. Most of the following historical information is based on Architectural Acoustics by Marshall Long (2006). 1 2 BERANEK, Leo, Concert Halls and Opera Houses, USA, Springer-Verlag New York, 2004, page 8ff. KAHLE, Eckhard, Kahle Acoustics, lecture at the EPFL, Switzerland, the 4th of november 2009. 6 1.2. Greek and Roman period (650BC - 400AD) Chant or theater plays with a supporting chorus were the main attraction for early performance spaces. 1.2.1. Theater and odea Theater (500BC - 0AD) An outdoor stone construction with a semi circular seating pattern was the first constellation of sound space that was conceived by Greeks and later also used by Romans for acoustical performances. This shape as many people as possible to assemble around a central area (see Fig. 01). Odea (0 - 450) Later, Greek playwrights depended more on the spoken dialogue than on the chorus. These performances were staged in small wooden indoor theaters, called odea, which had a capacity of about 200 to 1500 seats and assured good speech intelligibility with an elliptical seating arrangement (see Fig. 02). 1.2.2. Early acoustical knowledge People at that time didn’t know a lot about acoustics and almost everything they knew was based on empirical studies and assumptions. There are several known researchers who were investigating acoustical problems, -500 7 Chapter 1: History Of Sound Space 0 500 but there was one in particular who left us with some very practical information about how sound space had to be conceived: Vitruvius Pollio His book called De Architectura, which dates from around 27 BC, describes numerous aspects of contemporary theater design. Unrestricted sightlines and good speech intelligibility were apparently the main purposes of architects at that time. He also mentioned that seating should never face south to prevent the audience from having to look into the sun. 10 0 20 40 10 Fig. 01: Semi circular seating pattern 20 40 Fig. 02: Truncated elliptical seating of early theater design. 1000 0 arrangement. 1500 2000 8 1.3. Early Christian period (400 - 800) Performance style of this period was mostly religious chant. 1.3.1. Church Most known churches during that period had facades with ornamented marble. Neither the typically rectangular shape nor the materiality and texture of churches were particularly destined for acoustical performance (see Fig. 03). 1.3.2. Monody As explained in the introduction part of this chapter, religious church music had to adapt to those highly reverberant stone constructions, which is why they lowered their pace and used only a single melodic line with instrumental accompaniment, called monody.1 Even a simple line will be transformed into a beautiful blending of sound due to countless reflections from sidewalls and the ceiling. 1 http://en.wikipedia.org/wiki/Monody, visited 22.12.2009, 19:22. -500 9 Chapter 1: History Of Sound Space 0 500 1.4. Romanesque Period (800 - 1100) Religious chant remained popular in this period. 1.4.1. Church During the Romanesque period the main construction materials were brick, stone and ceramics, as well as scavenged materials from the Roman ruins. Compared to earlier buildings, decorative marble was used no more. 1.4.2. Organum A music style with two melodic lines, called organum, slowly began to develop. 10 0 20 40 60 80 100 Fig. 03: Rectangular church space without particular seating arrangement. 1000 1500 2000 10 1.5. Gothic period (1100 - 1400) Religious chant was still the main performance style during the Gothic period. 1.5.1. Gothic cathedral Construction materials stayed the same but interior space was liberated due to exterior support structures. 1.5.2. Plainchant, polyphony and miracle play Plainchant The beginning of the Gothic period was characterized by plainchant1, which still consisted in one single melodic line, but without instrumental accompaniment. Polyphony During the end of the twelfth century, the first polyphonic music was elaborated and started to get popular. Miracle and mystery play Public entertainment became less religious and more secular with the rise of towns and commerce. Miracle and mystery plays, which were 1 http://en.wikipedia.org/wiki/Plainsong, visited 22.12.2009, 19:26. -500 11 Chapter 1: History Of Sound Space 0 500 a combination of singing and spoken dialogue, were tolerated by the church. Since they were in Latin and average citizens did not understand them, these plays were performed as a pedagogical tool on the open street. As mystery plays developed, they were performed increasingly in the local language and used as entertainment. In order to be clearly understood, they started to be performed in rooms. 1000 1500 2000 12 1.6. Renaissance (1400 - 1600) Religious music was still dominating, but secular music became more and more popular. 1.6.1. Renaissance church and theater Renaissance Church Not only music was developing, but also the construction of various church designs were flourishing. Renaissance Theater In Italy, theater construction began more or less where the Romans had left it a thousand years ago (see Fig. 04). Later, small open-air theaters appeared in England, which provided adequate speech intelligibility due to beneficial early reflections of the sidewalls and the roof on top of the stage. The lack of a roof over the seats prevented reverberation problems. Outside noise was shielded by the high walls. Fig. 04: Elliptical seating arrangement of typical italian theaters during the Renaissance period. -500 13 Chapter 1: History Of Sound Space 0 500 1000 1500 2000 14 1.7. Baroque period (1600 - 1750) During this period, secular music became popular and also instrumental music gained more importance. 1.7.1. Baroque church, theater and opera Baroque Church More attention was attributed to the ornamentation of churches than during the Renaissance. Baroque Theater and Opera Seating became U-shaped in order to allow the patrons a view not only of the stage, but also of the prince whose seat was located on the centerline (see Fig. 05). The first standard for opera houses built in Venice were also U-shaped, but multistory seating arrangements (see Fig. 06), which further evolved into truncated elliptical shapes later on. Fig. 05: U-shaped seatings of Fig. 06: Italian opera houses also baroque theater design. -500 15 Chapter 1: History Of Sound Space featured an U-shaped, but multistory, seating arrangement. 0 500 1.7.2. Speech, Baroque and instrumental music Speech For Protestants in northern Europe, the spoken word was important for the religious service they offered. New churches were built with reduced volumes and old churches were modified with galleries and hanging draperies so that they offered small compartments in which good speech intelligibility was assured. Baroque music This music style abandoned the polyphony of sacred music in order to come back to a solo singer with a single instrumental support. Instrumental music Concerning theatrical performances, newly introduced moveable stage machinery made a lot of background noise, which had to be covered with instrumental music. That is why a lot of development had been made regarding different instrument types and loudness in order to satisfy the needs. 1000 1500 2000 16 1.8. Classical period (1750 - 1825) Classical music and operas were the main acoustical attractions during this period. 1.8.1. Concert hall and opera Concert hall For the first time in history, music was composed with a formal concert hall performance in mind. Early sound spaces were rarely built for that sole purpose. Concert halls of this period were mostly small rectangular halls with a seating capacity ranging from 400 to 600 people (see Fig. 07). Opera house The opera remained the center of cultural world in Italy. La Scala became the archetype of opera houses for the next two centuries. Its shape is similar to a horseshoe and small boxes are lining the walls like a layer cake (see Fig. 08). 1.8.2. Classical music Classical music can be characterized as being very strict in a sense that composers had to put careful attention to specific forms. -500 17 Chapter 1: History Of Sound Space 0 500 10 0 20 40 Fig. 07: First rectangular concert hall shapes. 10 0 20 40 Fig. 08: Horseshoe-like shape of the La Scalla with multistory seating arrange- ment as seen in previous opera house designs. 1000 1500 2000 18 1.9. Romantic period (1825 - 1900) It is difficult to precisely define the separation between the two time periods of Classical and Romantic. There are, however, some differentiations that can be made between the music and architecture of those. 1.9.1. Shoebox halls This rectangular shape type is still used nowadays. The most appreciated halls date from this time period. They are narrow, built with thick plaster and heavy wood, with a deeply coffered ceiling about 15 meters high. The floor is generally flat and the orchestra is seated above the patrons. There are different elements that help diffuse the sound such as chandeliers, highly ornamented sidewalls, overhanging balconies and recessed windows (see Fig. 09 and Fig. 10). 1.9.2. Romantic music and acoustical knowledge Romantic music Compared to classical music, Romantic music can be described as more personal and less constrained by a formal style. Acoustical knowledge The development of louder instruments encouraged the construction of larger concert halls and the use of full orchestras. This resulted in a less fa- -500 19 Chapter 1: History Of Sound Space 0 500 Fig. 09: Image of the Musikvereinssaal in Vienna as an example of romantic period’s halls. © by Jason7825 on Wikimedia vorable performance, since excessive reverberation time and long-delayed reflections significantly decreased the overall acoustical experience. Most efficient halls were designed using incremental changes from existing successful spaces. Unsatisfactory rooms were renovated or simply destroyed and eventually rebuilt with a new design. 10 0 20 40 Fig. 10: Narrow shoebox shape with short, overhanging balconies. 1000 1500 2000 20 1.10. Modernity (1900 - today) Today, concert halls are the most significant acoustical buildings that are built. As spectator numbers are still increasing, even more attention has to be paid on acoustical behavior of new room designs. 1.10.1. Concert halls and theaters With the increased possibility to create a more accurate forecast analysis for acoustical performance of concert hall and theater designs, there exists multiple shapes and materializations that result in good acoustical spaces. Compared with theaters, concert halls are longer with narrow balconies, whilst theaters have a short depth and a high ceiling. 1.10.2. Modern acoustics Since it seems that even modern spectators of concerts and theaters prefer how music sounded a hundred years ago, it is now up to architects and acousticians to create space which suits existing compositions1. This is why there is a lot of architectural research being conducted to satisfy the respective acoustical needs of concert halls and opera houses. 1 BERANEK, Leo, Concert and Opera Halls - How they sound, USA, Acoustical Society of America, 1996, page 16ff. -500 21 Chapter 1: History Of Sound Space 0 500 Wallace Clement Sabine Around 1900, Wallace Clement Sabine discovered that the product of the total absorption (A) and the volume (V) of a given space was a constant. He derived from this discovery the famous formula for reverberation time (T60, see (04)). (04): Reverberation time formula: T60 = 0.161 V/A [m] Leo Beranek Beranek’s contribution to modern acoustic theory was a first attempt of defining quantifiable acoustical attributes for concert halls. He is still one of the leading researchers of architectural acoustics today. Besides the two scientists mentioned here, there are numerous gifted scientists who are trying to get behind the mysteries of sound in architecture, some of them can be found in the bibliography of this paper (see “References” on page 181). 1000 1500 2000 22 analysis CHAPTER 02 2. ACOUSTIC SPACE ANALYSIS In this chapter, I will be focusing on analyzing the rules that created those different geometries we know of. In order to understand the development of shapes that are capable of producing good acoustics without help of electronic equipment, I have compared plans and sections of a number of spaces depending on the following criteria: 2.1. Selection samples The halls are chosen based on their importance of historical impact or their degree of popularity amongst musicians because of their acoustical properties. Since this work has already be done by professional researchers, I was satisfied with using the selection of Leo Beranek (1996) and Marshall Long (2006), who are listed in the reference section of this book (see “References” on page 181). I have added by myself the missing halls from Switzerland, because of my proper interest of having them included within this work. 2.1.1. Concert halls and opera houses of the world A selection raises the question of the importance of the sample items compared to the total pool of existing halls. This is why I have visualized all known concert halls and indoor theaters as listed on Wikipedia in diagrammatic form (see Fig. 11 to Fig. 12). Even if wikipedia cannot be considered as the most reliable source of information, still, it was the most 27 complete list I have found and I think the degree of reliability is high enough for this purpose. Concert halls 1% 19% africa asia africa europe asia europe oceania america oceania 48% america 30% TOTAL: 437 3% Fig. 11: Concert halls of the world with more than 1000 seats, as listed on http://en.wikipedia.org/wiki/List_of_concert_halls, visited 24.11.2009, 16:45 Opera houses 20% africa 2% 3% asia europe africa 3% asia europe oceania oceania america america TOTAL: 337 Fig. 12: Theaters of the world, as listed on 73% http://en.wikipedia.org/wiki/List_of_opera_houses, visited 24.11.2009, 16:45 28 Chapter 2: Acoustic Space Analysis We can state that there are quite more concert halls than indoor theaters in total. A large percentage of theaters in the world are built in the Europe, which is due to the concentration of opera houses in Italy about 500 years ago, from where theater construction spread its popularity towards France and Germany. 2.1.2. Selected concert halls and theaters Merging those two previous graphs into each other, we get another diagram (see Fig. 13) showing the overall dispersion of important interior music space over the world. Compared to Fig. 14, which is a visualization of selected spaces for this work, it gets clear that the samples chosen represent only about 10% of totally existing constructions of this type, but since only well known halls got into the selection, I think this analysis will still give a representative result of shape development over time. The distribution over the continents seems to be correlating between selection and total repartition, although there are more chosen halls within the Europe because of subjective selection of some single European samples. 29 Concert and opera halls 1% 12% africa 36% asia africa europe asia oceania europe oceania america TOTAL: america 774 49% 3% Fig. 13: Repartition of concert halls and opera houses over the five continents. Chosen halls for shape analysis 0% africa 10% 30% asia africa asia europe europe oceania america TOTAL: oceania america 3% 80 58% Fig. 14: The selected concert halls and opera houses for this shape analysis. 30 Chapter 2: Acoustic Space Analysis In order to compare shape development during time where symphonic concerts were not yet invented and theaters were performed mainly outside, there are ten shapes which are added to the eighty ordinary concert halls and opera houses. That makes a total number of ninety shapes that are analyzed in the following sections. Please refer to “Appendix : Schemes” on page 85 for the whole library of the sampled halls at scale. The following part can be considered as a graphical or geometrical approach of the previous chapter (see “History of Sound space” on page 4), which explained the history of spectacle halls in a more narrative way. 2.2. Type analysis Depending on the form of a room, there are different performance types that were typically enacted in it. This analysis gives us information about how those shapes changed in time and based on the type of spectacle that was popular at a specific period. There are three types that can be differentiated: song, theater and concert: Song This performance type consists in one or several vocalists that can be supported by instruments. There are different styles of song such as religious Song or pop music. 31 song theater concert 500BC - 0 32 0 - 500 500 - 1000 1000 -1500 Chapter 2: Acoustic Space Analysis 1500 - 1900 1900 - 2000 Fig. 15: Type analysis diagram with three categories: song, theater and concert. 33 Theater A theater can also be defined as a play, a representation of a story in musical form. There are several types of theaters that are performed today: drama, musical theater and comedy. Concert This art form is a performance style which uses instruments as main sound source. A story can be told in tonal form. 2.2.1. Comments for the type analysis diagram On the upper part of the type analysis diagram (see Fig. 15), there are floor plans of churches, which were the main acoustical spectacle spaces during more than a thousand years. Their shape was not that important for acoustics, since it was mainly due to the reflective interior surfaces that the sound got a lot of reverberation, which is characteristic for church music. Since my preoccupation is more of a geometric interest, I will leave out those floor plans for the following shape analysis. Concerning development of theaters and concert halls, this diagram gives us visual affirmation of historical facts that were described in the historical part of this book: Theaters were understood as semi circular outdoor spaces more than two thousand years ago. Around 1500, theaters got more popular again and those round seating arrangements were reused in rectangular interior spaces. Other curved forms like elliptical and U-shaped arrangements were tried out, which eventually resulted in a horseshoe shape, which got 34 Chapter 2: Acoustic Space Analysis a reference until about 1950. Today, we have an increasing number of fan shaped theater constructions. Concert halls started their history much later on with simple rectangular shapes. As symphonic concerts gained more popularity, other geometries like the fan shape got more common. With advancing knowledge in acoustical behavior, other geometries like diamond, asymmetrical and even elliptical shapes were experimented. Those reflections on form lead us to the next analysis, which treats the question of shape development. 2.3. Shape analysis The arrangement of the sample schemes into defined geometries is not a task that can be done without subjective decisions. Forms that were quite defined earlier got diversified within the last hundred years.1 This is why I am giving a short description of my understanding of existing forms. This definition does not completely go with Beranek’s (1996) classification of form. It is to mention that he did not pursue this designation in his future work (Beranek, 2004). Nevertheless, I think it will be useful for my personal project to have them sorted by form and seating arrangement as a classified library of precedents (see Fig. 23). My form categories present itself as follows: 1 BARRON, Michael, Auditorium Acoustics and Architectural Design, England, E & FN Spon, 1993, page 47f. 35 Rectangular Also referred as “shoebox” form, it can be considered as the most standard and secure concert Fig. 16: Rectangular shape hall shape that exists today because of the close sidewalls that give every listener an enveloped impression due to early reflections. Semi circle / Semi elliptic This seating arrangement was experimented a lot during the beginning of spectacle place construction. They are the most efficient forms Fig. 17: Semi circle and semi elliptic shape to assemble a big number of people around a single stage. Fan In its pure form, it is considered as less efficient than a rectangular shape, since important lateral reflections lose of their strength. Fig. 18: Fan shape I considered a hall being fan-shaped as soon as sidewall opened itself towards the back of the room. Exceptions to this rule are the following: Horseshoe A typical shape for theaters. The concave back wall concentrates sound in its focus point, 36 Chapter 2: Acoustic Space Analysis which creates a bad balance of sound intensity. Thus, it is not recommended for concert halls. For this geometry, seating area forms one Fig. 19: Horseshoe shape single curve starting on one side of the concert hall and ending on the other side. Diamond This more recent variation of the fan shape represents a compromise between its visual effect and the efficiency of enclosure of a rectangular Fig. 20: Diamond shape shape that is achieved with the reverse splay. Elliptic This form is acoustically one of the worst form that exists, because of its two focal points. But still, acoustics can be enhanced by breaking ori- Fig. 21: Elliptic shape entation of the circumfluent walls. This technic is used in more modern halls. Freeform / Asymmetric These are the most liberated shape categories and also the most modern. Research in architectural acoustics is already that advanced that it is possible to get satisfactory sound propagation Fig. 22: Freeform shape for almost every imaginable form. 37 rectangular semi circle / semi elliptic / fan horseshoe diamond / elliptic asymmetric / freeform 500 BC 38 1500 - 1900 Chapter 2: Acoustic Space Analysis 1900 - 1950 1950 - 2000 Fig. 23: Shape analysis diagram comparing different geometries. 39 2.4. Seating arrangement Another possible classification of the plan schemes is the configuration of seating areas (see Fig. 26) in concert halls. I split them up in the following three categories: Frontal A frontal seating arrangement represents the acoustically most favorable seating pattern. Side- and back walls close to the stage help creating early reflections that enhance the sound experience within the whole room. Lateral Lateral seats can be interesting to spectators to see the orchestra from another point of view, but on the cost of a well balanced sound (see Fig. 24). The balustrade on the other hand can be used to reflect sound towards the main part of the hall. Circumfluent Circumfluent arrangements are created by pushing away the back wall of the scene in order to create space for spectators. Sound intensity towards the main part of the hall weakens considerably, but the visual experience for people seated behind the scene can be quite haunting (see Fig. 25). 40 Chapter 2: Acoustic Space Analysis Fig. 24: Photograph of the Musikvereinssaal in Vienna, Austria. ©by XarJ’s blog Fig. 25: Image of the Kammermusiksaal in Berlin, Germany. ©philharmonie.com, Inc. 41 frontal lateral circumfluent 1800 - 1900 42 Chapter 2: Acoustic Space Analysis 1900 - 2000 1950 - 2000 Fig. 26: Seating arrangement diagram with three categories: frontal, lateral and circumfluent. 43 2.5. Section analysis The same type analysis I did in plan, can also be done in section (see Fig. 33). I used the same arrangement as for Fig. 15 on page 33, which makes the two graphs directly comparable. 2.5.1. Section types A general reflection of section development is illustrated on the right hand side (see Fig. 27 to Fig. 32). In order to perform something in front of a mass of people, the first idea was to raise the scene (see Fig. 27). By sloping the seating space, even more people could see the scene (see Fig. 28). Later on, it was recognized that a back wall for the scene enhanced the sound intensity towards spectators (see Fig. 29). An enclosed scene reflected even more sound waves to the seating area (see Fig. 30), whilst obviously the enclosed space finally was the best solution for capturing every sound that is produced on the scene (see Fig. 31). A contraction of the volume above the scene (see Fig. 32) does not add considerably to the overall intensity of sound arriving at the listener, but it enhances the ratio between early arriving sound waves and later reflections. This is an appreciated factor for spectators, which will be discussed in the following chapter (see “3.2. Measurable parameters” on page 56).1 2.5.2. Comments for the section analysis diagram The later sections of the rooms used for music performances show very clearly the separate reverberant fields that are created below the different 1 44 CAVANAUGH & WILKES, William & Joseph, Architectural Acoustics - principles and practice, USA, John Wiley & Sons Inc., 1999, page 154. Chapter 2: Acoustic Space Analysis Fig. 27: raised scene domes, but otherwise, there is no geometric setting that helps sound propagation towards the spectators. Compared to concert hall sec- Fig. 28: sloped seating tions, the diagrams of theaters are generally higher and shorter. Since a play not only needs to be heard, it is also favorable to be as close as possible to the scene. This is prob- Fig. 29: backwalled scene ably the main reason of the different proportions. Another explanation could be the stage tower, which had to be quite high anyway. Opera diagrams are very similar Fig. 30: enclosed scene especially during the period where Milan’s most famous opera house La Scala was perceived as the reference for theater construction. Its main characteristics in section is Fig. 31: enclosed space the back wall covered with recessed balconies. As for concert halls, compared to the very first precedents, major modifications have happened in Fig. 32: contracted scene space treatment of roof structure. The 45 song theater concert 500BC - 0 46 0 - 500 500 - 1000 1000 -1500 Chapter 2: Acoustic Space Analysis 1500 - 1900 Fig. 33: Section analysis diagram with three categories: song, theater and concert. 47 ceiling of earlier halls were flat or had regular cavities. Later halls are taking advantage of modern research and techniques by applying oriented panels, convex shapes or other sound dispersing forms. Another point to mention are the reflector panels that are suspended inside the volume. Most of the time, they were installed later on as objects of a renovation. 2.6. Conclusion of the analysis Looking at those diagrams, we could suppose that there is a diversification of shape in the last hundred years. But it has to be said that we do not have evidence of every sound space that has been built over history. This means that already the Greeks two thousands of years ago, they for sure experimented with their own forms that were less successful. They were destroyed, rebuilt or modified and hence, they did not survive until today. I think by drawing all those diagrams, I started to get an idea of the development of those shapes and geometries. The next step would be to understand the physics behind, in order to be able to recreate them under different circumstances. 48 Chapter 2: Acoustic Space Analysis 49 acoustics CHAPTER 03 3. ARCHITECTURAL ACOUSTICS This chapter will be treating the acoustical parameters that led to those shapes I have analyzed in the previous chapter. As we have learnt from the historical part of this research, our knowledge in architectural acoustics is already that advanced that we are no more restricted in strictly rebuilding former concert hall designs (see “Concert halls and theaters” on page 21). This gives us architects the liberty to design new shapes with similar acoustical properties to other successful halls that were built previously. There are some rules though that have to be applied which will be explained in this chapter. 3.1. Fundamentals of acoustics Before entering into more complex parameters of architectural acoustics, I would like to briefly introduce some fundamental characteristics of sound. 3.1.1. Physical definition of sound A sound is an oscillation of pressure transmitted through a solid, liquid or gas.1 This difference of pressure is generally very small compared to atmospheric pressure, but still, it can be perceived by our ears and translated into sound. 1 http://en.wikipedia.org/wiki/Sound, visited 02.01.2010, 16:04. 53 3.1.2. Representations of a single sound wave Sound propagates in a longitudinal form (see Fig. 35). However, it can be represented as a transverse wave (see Fig. 34) by plotting x-axis values on the y-axis. Representing a sound as a transverse wave gives us the possibility to visualize its amplitude and frequency. amplitude frequency Fig. 34: Sound wave representation Fig. 35: Sound represented as as transverse wave. longitudinal wave. 3.1.3. Representation of multiple sound waves Normally, a sound can be referred as being multiple waves that add up to a single level of pressure that can be measured in time. A representation of such a curve is shown in Fig. 36. For certain parameters it is more readable to only visualize the impulses that arrive at a certain point, which is sound pressure level sound pressure level represented in Fig. 37. time Fig. 36: Sound measurement represented as curve. 54 Chapter 3: Architectural Acoustics time Fig. 37: Sound measurement represented as arriving impulses. 3.1.4. Frequency The frequency of a sound is defined as the number of compressions per seconds. The unit used to measure frequency is named Hertz. This term is important for architectural acoustics because it is determining how a sound is absorbed when arriving on a surface. 3.1.5. Absorption and reflection Those two attributes are contributing to the complexity of sound propagation models. Because absorption and reflection of different frequencies vary depending on the incident angle of a sound wave, perfectly accurate models are difficult to obtain. This is why an average value is used for defining the absorption coefficient. Generally we can say that sound waves of a high frequency, which signifies a short wavelength, are absorbed with porous materials with small holes such as fabrics.1 Waves with a longer wavelength are rather absorbed with panel or resonant absorbers. 3.1.6. Perception of sound Human aural system has the capacity to perceive sound of a large range of physical intensity. But whether we sense a sound as annoyingly loud or just correct depends on the listener itself and is hence very subjective. When we speak of ideal sound properties, it does mean that characteristics match the preference of the majority of potential or past listeners.2 1 2 LONG, Marshall, Architectural Acoustics, in: op. cit., pages 261ff. http://www.baunetzwissen.de/standardartikel/Akustik_Wahrnehmung-undEinflussfaktoren_147627.html, visited 02.01.2010, 19:28. 55 3.2. Measurable parameters In order to create rules that could drive the concert hall engine I would like to design, I need quantifiable parameters that are generally appreciated by the public. The following parameters are a selection of such measurable qualities of a room that I intend to use for future development of my project. 3.2.1. Reverberation time The most known parameter for concert hall design is the reverberation time. It designates the time required for the reverberant sound to decay by 60 dB of its maximum (see in “Appendix : Schemes” on page 85 for a more detailed explanation of this term). The optimal values are depending on the type of performance. They’re visualized in the following diagram (see Fig. 38). Organ Romantic classical Early classical Opera Chamber Drama (spoken word) 0.5 1.0 1.5 2.0 2.5 Fig. 38: Subjective reverberation time T60 (Occupied) preferences in seconds for occupied rooms, diagram derived from Barron (1993), page 29. 56 Chapter 3: Architectural Acoustics Reverberation time can be obtained easily with the formula of Sabine (05), which makes it a good parameter to control general acoustical properties of a room. (05): Reverberation time formula by Sabine: T60 = 0.161 V/A [m]1 V = total volume of the room. A = total absorptive area = α × ST α = absorption coefficient ST = total acoustic area (see page 85) 1 LONG, Marshall, Architectural Acoustics, in: op. cit., page 301. The correlation between reverberation time (T60), volume (V) and total acoustical area (ST) are visualized in Fig. 39. T60 (Occ) 1.6 1.7 1.8 3000 1.9 2.0 acoustical area ST in m2 2500 2000 1500 1000 0 10 15 20 25 30 35 40 room volume in 1000 m 3 Fig. 39: Chart for determining the Acoustical Area of a Concert Hall. This diagram is derived from Beranek (1996), page 448. 57 3.2.2. Loudness This parameter hardly needs any definition. A sound will be perceived much louder in a room with 10’000 m3 than in a room with 20’000 m3 that has a similar reverberation time. The following diagram visualizes this correlation using the terms already defined in the previous charts. “Loudness” is defined here as Gmid, which is explained more in detail in “Appendix : Schemes” on page 85. Using this term, 5 dB ±1 is about the preferred value for a concert hall.1 Gmid = 2 dB 35’000 room volume V in m3 30’000 Gmid = 3 dB 25’000 Gmid = 4 dB 20’000 Gmid = 5 dB 15’000 Gmid = 6 dB 10’000 1.6 1.7 1.8 1.9 2.1 2.2 reverberation time T60 (Occupied) in seconds Fig. 40: Chart for determining the volume of a concert hall, derived from Beranek (1996), page 447. 1 58 BERANEK, Leo, Concert and Opera Halls - How they sound, in: op. cit., page 446. Chapter 3: Architectural Acoustics 3.3. Number of seats Using those parameters it is possible to determine the actual seat count that goes with the desired acoustical properties of a room. In Long’s (2006) book on architectural acoustics there is a very neat summary from Beranek’s (1996) research on how this can be done, which I am going to quote as is: (06): [...] Beranek assumes that the audience and orchestra represent 75% of the total absorption in a hall and that the average midfrequency absorption coefficient is 0.85. The absorption area, ST (sq m), is the combined area of the audience and the orchestra times a factor of 1.1 to account for the side absorption. [...]1 1 LONG, Marshall, Architectural Acoustics, in: op. cit., page 678. These guidelines give us a new formula for reverberation time (07), which allows us to connect the previously discussed values with the actual seat number. (07): Adapted reverberation time formula: T60-o ≈ 0.14 (V / ST)1 1 LONG, Marshall, Architectural Acoustics, in: op. cit., page 678. 59 3.4. Further measurable parameters There are some more measurable parameters that are discussed amongst researchers on architectural acoustics. I did not yet find a way how to predict all of these efficiently in an engine that resolves problems in real-time, but maybe future work will treat them more in detail. 3.4.1. Intimacy This parameter can also be defined as “presence” of a hall and it designates the impression of music being played in a small hall rather than in a vast space.1 One quantifiable value that designates this rather subjective impression of intimacy is the initial-time-delay gap (tI). It is defined as the delay of the first reflection measured in the center of the main body of a room.2 This parameter can easily be obtained with geometric work on plan and section. B A sound pressure level A B initial-timedelay gap time Fig. 41: Geometric visualization for tI (initial-time-delay gap). A = direct sound B = first reflection 1 2 60 Fig. 42: Diagrammatic visualiza- tion for tI, derived from Barron (1993), page 40. BERANEK, Leo, Concert and Opera Halls - How they sound, in: op. cit., page 22f. in: ibid. page 511f. Chapter 3: Architectural Acoustics 3.4.2. Warmth “Warmth” in music can be defined as the ratio between the fullness of the bass tones (between 75 and 350 Hz) to that of the mid-frequency tones (350 to 1’400 Hz), which is also the definition to the term “bass ratio”, as explained in the “Appendix : Schemes” on page 85.1 This means in practice that a hall should have some bass reverberation creating surfaces in order to be perceived as “warm”. This kind of reverberation in these low frequency tones are obtained with very heavy materials such as 50 mm thick wood on a concrete plaster backing. Fig. 43 does visualize how reverberation time at lower frequencies should ideally increase in percentage of the value at 1’000 Hz. percentage of value at 1’000 Hz 160 150 140 130 120 110 100 65 125 250 500 1’000 2’000 4’000 frequency, Hz Fig. 43: Ratio of the bass to mid-frequency reverberation time. Diagram derived from Long (2006), page 587. 1 in: ibid. page 23f. 61 3.4.3. Envelopment A factor that I considered as quite interesting which contributes to “Envelopment” is the surface diffusivity index (SDI). There is general agreement that diffusivity is good, since it helps to envelope a listener with reverberant sound coming evenly distributed from different directions, but it is less defined how to measure it.1 As explained in “Absorption and reflection” on page 55, diffusion is difficult to quantify, because reflections of an arriving sound depend on the frequency and the incident angle and in addition to this, measurement needs to be performed at locations over the entire half-sphere surrounding the diffuser. A value of 1 designates a highly diffusive surface whilst 0 means low diffusivity. The highest value of one can be considered as the optimal value for this parameter. 3.5. Conclusion on architectural acoustics There are a lot of terms that imply an acoustical quality of sound. The parameters chosen are merely a fraction of what exists, but I tried to select those I could be capable to handle for the concert hall engine I would like to design. Every one of those parameters has also the capacity to serve as architectural concept, meaning combining acoustical with architectural characteristics. A hall that offers highly enveloping and intimate sound for example can go along with a seating arrangement that consists in embracing boxes that are spread throughout the space or a hall with “warm” sound 1 62 LONG, Marshall, Architectural Acoustics, in: op. cit., page 681. Chapter 3: Architectural Acoustics would also be built with warm materials such as wood and fabrics, having warm lighting or be painted in warm colors. These reflections lead us to the next chapter, which will treat the problematics of the proposition of a concert hall engine. 63 engine CHAPTER 04 4. CONCERT HALL ENGINE The aim of this concert hall engine is to support the design process of a concert hall. It should be a combination of help for resolving known acoustical problems and formulas and assistance or generator for shape and concept development. Time is constraining, which is why this engine does exist only in a very limited state yet. It is at least already capable of calculating the most simple equations that are mentioned in the previous chapter. In this part, I am going to explain my intentions concerning development of this engine and which possibilities it would offer. This chapter can also be considered as a pool of ideas. 4.1. Introduction to the engine Resumed in a phrase, the engine consists in three types of inputs (numeric, optional and graphical) that result in a mostly visual output that varies a lot depending on what I am intending to achieve with. Numeric input is a single value for the seat count, graphical input can be closed splines or polygons. Optional inputs are values for the selected acoustical parameters. Their range of preference is already defined inside the engine, but it can be overwritten by a manual input. There is also some numeric output that is used to calculate the visual data. For more detail, please refer to Fig. 44 on the next page. 67 GRAPHICAL INPUT »» total floor surface »» seating+circulation area »» stage area Visual Output Numeric Output Input NUMERIC INPUT »» number of seats 68 VALUE CALCULATION »» ideal average height »» ideal total volume »» volume per seat ratio » ideal absorption (ST) » ideal stage area » VOLUME STAGE AREA STAGE WALLS »» floor spline x height »» area per musician »» ideal primary reflections Chapter 4: Concert Hall Engine OPTIONAL INPUT »» »» »» »» »» reverberation time volume per seat ratio loudness (Gmid) orchestra size area per musician » input total floor surface » input seating+circulation area » input stage area BALCONY SECTION EMBRACING WALLS SEATING AREA »» section depending on depth »» splitting seating area into small parts »» seating+ circulation area Fig. 44: graphic representation of the concert hall engine. 69 4.2. The different applets of the engine I am giving a short explanation on the way those different proposed visual outputs (applets) would work. 4.2.1. Volume A fairly easy visualization which already works in the present applet, which consists in drawing the total volume as an extrusion from the input of the total floor area. 4.2.2. Stage area Taking the graphic input of stage area as reference, this applet would resize it according to the defined area per musician and the eventually defined size of the orchestra. 4.2.3. Stage walls This applet would calculate the orientation and form of the sidewalls in order to get ideal primary reflections towards the main seating area. The same thing could be done for reflections back to the stage to create a good “ensemble” (this term refers to the ability of the performers to play in unison1). The same operation can also be done in section, where the ideal angle and positioning of the existing roof or an overhanging canopy will be calculated. 1 70 BERANEK, Leo, Concert and Opera Halls - How they sound, in: op. cit., page 25. Chapter 4: Concert Hall Engine 4.2.4. Balcony section Depending on the design of the concert hall, it is possible that the room has no balconies. But in case I will be in need of profound overhanging balconies, it would be helpful to have a tool that helps applying the known rules for the design of balcony sections. There are several ways to reinforce the lack of sound in a profound room under balconies. This applet would apply them according to the proportions of this space. 4.2.5. Embracing walls This tool is assigned to a specific type of seating, which is the vineyardstyle seating arrangement. It would split the existing seating area into several smaller areas which are then shifted in height between each other in order to create close sidewalls for each of these areas that provide them with well appreciated early reflections. There is also the possibility to extend this applet in section with the idea that finally every existing surface in the hall is oriented such as those areas get ideal primary reflections. 4.2.6. Seating area A more or less similar tool regarding the segmentation of seating and circulation area. This applet would consist in splitting up the graphical input of total seating and circulation area into several accessible parts and eventually propose the creation of balconies, if the requested seating count does would be too important for the existing area. 71 4.3. Further extensions of the engine 4.3.1. Graphical input assistance At the moment, graphical input happens completely manually. There could be some kind of assistance or engine on its own that draw a floor line which is then fed into the engine. 4.3.2. Lower seat dependence Having to define a seat count in advance does constrain projects where there is fixed volume at disposition. A system that tracks back to the seat number and lowers it if necessary could be quite useful. This can also be done manually by trial and error. 72 Chapter 4: Concert Hall Engine 73 project CHAPTER 05 5. PARAMETRIC CONCERT HALL There are the assembled information and ideas that already exist concerning the actual project of a parametric concert hall that I will conduct as master project. 5.1. Site The actual site for this type of master project is not as essential as it may be for other projects, which is why there has been no detailed research on a site in this work. It is however important to put the project in a credible context. A way to resolve this lack of investigation of a site would be to choose a known perimeter which avoids having to do extensive research of the environnment. As already known by attentive members of the EPFL, there is a project on a future conference center with an auditorium for the EPFL that is being planified. There is only a few information available in public, but there is already a demand for changing the zone of the perimeter in question, which is represented in Fig. 45 on the next page. The blue perimeter designates the space the conference center complex will occupy. This perimeter would offer the advantage of an actual similar project that will be developed in parallel. My work could give an alternative proposition of an auditorium that would function also or only as a concert hall. 77 78 Chapter 5: Parametric Concert Hall 1 du : L’attestent : Le syndic à Ecublens Zone du domaine ferroviaire : Zone d'activité mixte du Forum nord Périmètre de l'addenda au : Etat de Vaud Etat de Vaud Renaud et Burnand SA ingénieurs géomètres officiels Av. de Préfaully 29, 1020 Renens Tél 021 634.04.81 Fax 021 634.74.32 Confédération Suisse DP 2 (Dép. des finances et des douanes) 1478 propriétaire Le secrétaire L'ingénieur géomètre breveté : Renens, le ETABLI SUR LA BASE DES DONNEES CADASTRALES DU 30.05.2007 735 116 63’351 surface comprise dans l’addenda (m2) Limite à la forêt, 10 m Délimitation de l'aire forestière selon constatation de nature du 11 juillet 2001 Aire forestière (indicative hors du périmètre) Zone de verdure à vocation écologique Zone ferroviaire étape 2 Zone ferroviaire 2 ECHELLE 1:1000 Soumis à l'enquête publique, Périmètre du PAC 229 LEGENDE DP 1000 n° parcelle 0730-Addenda1-PAC229-1000-120608-LO-pab Juin 2008 Lausanne, le Le Chef du Département : Approuvé par le Département compétent 3 Le chef de Service du développement territorial (SDT) : N ADDENDA 1 AU PLAN D’AFFECTATION CANTONAL N°229 Etat de Vaud Département de l’économie Fig. 45: Addenda 1 au plan d’affectation cantonal N°229 5.2. Program The construction of a concert hall does also need a program that goes with the main hall. In relation with the site and a proposition with a lower audience than planned, the following program could be applied: Perimeter (Dimensions: 45 m x 100 m) 4500 m2 Concert Hall audience 2000 seats length 35 m largeness 25 m height (max.) 15 m volume 14’000 m3 Scene 140 m2 Direction 14 m2 Public Foyer 300 m2 Entrance Hall 900 m2 1200 m2 1200 m2 Bars Services 79 Artists Foyer 150 m2 Cloak room 150 m2 Practice room 200 m2 Instruments Depot 100 m2 Personnel Studios 40 m2 Office 15 m2 Administration 650 m2 60 m2 100 m2 Office (Director, Artistic Director, Secretary, Cash office) Documentation Library 100 m2 50 m2 Listening room 25 m2 Technical rooms 400 m2 Depot Service access TOTAL 80 Chapter 5: Parametric Concert Hall 3700 m2 5.3. Design There are two concert hall designs that awakened my interest 5.3.1. Vineyard-style seating arrangement This type of seating arrangement was first used for the Berlin Philharmonie in Germany which received good critics. A main advantage of this seating type is to create an acoustically intimate atmosphere with the surrounding walls for every vineyard field by elevating successively adjacent plateforms. As explained in the previous chapter treating the concert hall engine( see “Embracing walls” on page 71), it could be interesting to investigate further in an engine that tries to orient every existing surface in a hall towards one of these plateforms. 5.3.2. Diamond form As previously explained (see “Diamond” on page 37), this form is a good compromise between the acoustical advantage of the rectangular and the visual effect of the fan form. I thought it could be intersting to proceed further with refining this concept of synthesizing acoustics and visuals interior surface design and materiality. 81 appendix APPENDIX : SCHEMES All concert hall shape samples are listed in chronological order of their inauguration and with the same scale (1/1’000), except for schemes 0330 and 1220. Details of each hall are given when available. I used the following abbreviations: Type = performance type of the sample : song, concert or theater. Shape = shape of seating area or the surrounding walls : rectangular, semi elliptic, semi circular, fan, horseshoe, diamond, elliptic, freeform or asymmetric. Reverberation time = RT. This is the most recognizable acoustical parameter associated with concert halls. It is defined as the time required for the reverberant sound to decay by 60dB of its maximum.1 It is defined as the time, multiplied by a factor of 2, that it takes for the sound in a hall to decay from -5 to -35 dB below its steady-state value. V = volume of a hall. H = average height. W = average width. L = average length, mesured from the front of the stage to the backwall. Sa = area of projected floor space over which the audience chairs are located. 1 LONG, Marshall, Architectural Acoustics, in: op. cit., page 674. 85 SA = acoustical audience area. This parameter adds to Sa a strip of 0.5 m around seating areas where the border is exposed and capable of absorbing incoming sound waves. SO = are of stage or pit. ST = SA + SO 1 - IACCE3 = interaural cross-correlation coefficient. Measure of the difference in the sound arriving at the two ears of a listener facing the performing entity in a hall. IACCE3 is determined for a time period of 0 to 80 msec. It is the averages of the values measured in the three octave bands with mid-frequencies of 500, 1’000 and 2’000Hz. This coefficient is a sensitive measure to determine the apparent source width of a performing entity as heard by a person seated in the audience. This parameter correlates with the subjective impression of “spaciousness”. EDT = early-decay-time. It is comparable to RT except that EDT is obtained with the measure of time it takes for a signal to decay from 0 to -10dB. In order to be comparative to RT, the measured value is multiplied by 6. SDI = surface diffusivity index. This value indicates the diffusivity of a surface, 0 being the lowest and 1 being the highest value = highly diffuse. Gmid = the mid-frequency “strength factor”. It is the ratio, expressed in decibels, of the sound energy at a seat in a hall that comes from a non-directional source to the sound energy from the same source when measured in an anechoic room at a distance of 10 m. Gmid is defined as the average of the 125 and 250 Hz bands. It correlates to the subjective impression of "loudness". 86 Appendix : Schemes tI = initial-time-delay gap. It is defined for Beranek’s book (1996) as the time interval in msec between the arrival at a seat in the middle of the main floor of the direct sound from a source on stage to the arrival of the first reflection. This parameter correlates with the subjective impression of “intimacy”. BR = bass ratio. This parameter is the ratio of two reverberation times for an occupied hall. The denominator is the average of the RTs at 500 and 1’000 Hz and the numerator is the average of the RTs at 125 and 250 Hz. It can also be defined as “warmth” of a sound. Detailed description of these terms are derived mostly from Beranek (1996), page 47, 513, 457f, 567ff. Schemes and values that will follow are redrawn from the following ressources: • BARRON, Michael, Auditorium Acoustics and Architectural Design, England, E & FN Spon, 1993. • BERANEK, Leo, Concert and Opera Halls - How they sound, USA, Acoustical Society of America, 1996. • BERANEK, Leo, Concert Halls and Opera Houses, USA, Springer-Verlag New York, 2004. • CLASIEN, Delphine, Une salle de concert à Maastricht, Lausanne, Projet de Master EPFL, 1997. • LONG, Marshall, Architectural Acoustics, USA, Elsevier Academic Press, 2006. 87 -0330 Theater at Epidaurus Epidaurus, Greece 0 Type : Theater Shape : Semi circle Seats : 17’000 Voulme : Height : Length : 80 m Width : 120 m Reverberation t : - 88 Appendix : Schemes 10 V / ST : V / SA : V / N : SA / N : H / W : L / W : 0.7 So : Sa : - 30 SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - -0330 Theater at Epidaurus Epidaurus, Greece 0 Type : Theater Shape : Semi circle Seats : 17’000 Voulme : Height : Length : 80 m Width : 120 m Reverberation t : - 10 V / ST : V / SA : V / N : SA / N : H / W : L / W : 0.7 So : Sa : - 30 SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 89 -0012 Odeon of Agrippa Athens, Greece 0 Type : Theater Shape : Semi elliptic Seats : 200-1500 Voulme : 18750 m3 Height : 25 m Length : 30 m Width : 25 m Reverberation t : - 90 Appendix : Schemes 10 V / ST : V / SA : V / N : SA / N : H / W : 1.0 L / W : 1.2 So : Sa : - 30 SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 0080 Theater at Aspendum Aspendum, Turkey 0 Type : Theater Shape : Semi circle Seats : Voulme : Height : Length : 50 m Width : 80 m Reverberation t : - 10 V / ST : V / SA : V / N : SA / N : H / W : L / W : 0.6 So : Sa : - 30 SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 91 0330 Church of St. Peter Rome, Italy 0 20 Type : Song Shape : Rectangular Seats : huge Voulme : 1’188’000 m3 Height : 60 m Length : 180 m Width : 110 m Reverberation t : long 92 Appendix : Schemes 40 V / ST : V / SA : V / N : SA / N : H / W : 0.5 L / W : 1.6 So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 0530 Church of St. Sophia Constantinople, Turkey 0 Type : Song Shape : Orthogonal Seats : Voulme : 196’000 m3 Height : 40 m Length : 70 m Width : 70 m Reverberation t : long 10 V / ST : V / SA : V / N : SA / N : H / W : 0.6 L / W : 1.0 So : Sa : - 30 SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 93 1140 Basilica di San Marco Venice, Italy 0 Type : Song Shape : Orthogonal Seats : Voulme : 78’500 m3 Height : 35 m Length : 50 m Width : 50 m Reverberation t : long 94 Appendix : Schemes 10 V / ST : V / SA : V / N : SA / N : H / W : 0.7 L / W : 1.0 So : Sa : - 30 SA :ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1200 0 20 Type : Song Shape : Rectangular Seats : 9’000 Voulme : 162’000 m3 Height : 30 m Length : 120 m Width : 45 m Reverberation t : long Cathédrale Notre-Dame de Paris Paris, France 40 V / ST : V / SA : V / N : SA / N : H / W : 0.7 L / W : 2.7 So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 95 1580 Teatro Olympico Vicenza, Italy Type : Theater Shape : Semi elliptic Seats : Voulme : Height : Length : Width : Reverberation t : - 96 Appendix : Schemes V / ST : V / SA : V / N : SA / N : H / W : L / W : So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1588 Type : Theater Shape : Horseshoe Seats : s mall Voulme : Height : Length : Width : Reverberation t : - Teatro Sabbioneta Sabbioneta, Italy V / ST : V / SA : V / N : SA / N : H / W : L / W : So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 97 1620 Teatro Farnese Parma, Italy Type : Theater Shape : Horseshoe Seats : s mall Voulme : Height : Length : Width : Reverberation t : - 98 Appendix : Schemes V / ST : V / SA : V / N : SA / N : H / W : L / W : So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1637 Type : Theater Shape : Horseshoe Seats : Voulme : Height : Length : Width : Reverberation t : - Teatro di Giovanni e Paolo Venice, Italy V / ST : V / SA : V / N : SA / N : H / W : L / W : So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 99 1776 Stadtcasino Basel, Switzerland 0 Type : Concert hall Shape : Rectangular Seats : 1’448 Voulme : 10’500 m3 Height : 15.2 m Length : 23.5 m Width : 21 m Reverberation t : 1.8s 100 Appendix : Schemes 10 30 V / ST : 11.8 m V / SA : 14.4 m V / N : 7.25 m3 SA / N : 0.50 m2 H / W : 0.72 L / W : 1.12 So : 160 m2 Sa : 584 m2 SA : 731 m2 ST : 891 m2 1-IACCE3 : 0.64 Decay time (EDT) : 2.0s Diffusivity (SDI) : 0.8 Loudness (G mid) : 6.6dB Intimacy (tI) : 16 msec Warmth (BR) : 1.17 1778 Teatro alla Scala Milan, Italy 0 Type : Theater Shape : Horseshoe Seats : 2289 Voulme : 11’252 m3 Height : 19.2 m Length : 30.2 m Width : 20.1 m Reverberation t : 1.2s 10 V / ST : 6.9 m V / SA : 8.65 m V / N : 4.92 m3 SA / N : 0.57 m2 H / W : 0.95 L / W : 1.5 So : 125.4 m2 Sa : - 30 SA : m2 ST : 1’635 m2 1-IACCE3 : 0.48 Decay time (EDT) : 1.2s Diffusivity (SDI) : Loudness (G mid) : 1.4dB Intimacy (tI) : 20 msec Warmth (BR) : 1.21 101 1821 Konzerthaus Berlin Berlin, Germany 0 Type : Concert hall Shape : Rectangular Seats : 1’575 Voulme : 15’000 m3 Height : 17.7 m Length : 24.1 m Width : 20.7 m Reverberation t : 2.0s 102 Appendix : Schemes 10 30 V / ST : 13.6 m V / SA : 15.9 m V / N : 9.53 m3 SA / N : 0.60 m2 H / W : 0.85 L / W : 1.16 So : 158 m2 Sa : 784 m2 SA : 943 m2 ST : 1’101 m2 1-IACCE3 : 0.66 Decay time (EDT) : 2.2s Diffusivity (SDI) : 1.0 Loudness (G mid) : 5.5dB Intimacy (tI) : 25 msec Warmth (BR) : 1.23 1857 Mechanics Hall Worcester, USA 0 Type : Concert hall Shape : Rectangular Seats : 1’343 Voulme : 10’760 m3 Height : 12.5 m Length : 27.1 m Width : 24.7 m Reverberation t : 1.55s 10 V / ST : 12.5 m V / SA : 15.4 m V / N : 8.01 m3 SA / N : 0.52 m2 H / W : 0.51 L / W : 1.1 So : 154 m2 Sa : 541 m2 30 SA : 701 m2 ST : 855 m2 1-IACCE3 : 0.57 Decay time (EDT): 2.2s Diffusivity (SDI) : 0.8 Loudness (G mid) : 5.6dB Intimacy (tI) : 28 msec Warmth (BR) : 1.16 103 1858 Royal Opera House London, Great Britain 0 Type : Theater Shape : Horseshoe Seats : 2’120 Voulme : 12’250 m3 Height : 18.6 m Length : 29.9 m Width : 24.4 m Reverberation t : 1.1s 104 Appendix : Schemes 10 30 V / ST : 7.67 m V / SA : 9 m V / N : 5.8 m3 SA / N : 0.64 m2 H / W : 0.76 L / W : 1.2 So : 62.2 m2 Sa : 1’090 m2 SA : 1’360 m2 ST : 1’600 m2 1-IACCE3 : Decay time (EDT): 1.1s Diffusivity (SDI) : Loudness (G mid) : 1.2dB Intimacy (tI) : 18 msec Warmth (BR) : 1.07 1870 Grosser Musikvereinssaal Vienna, Austria 0 Type : Concert hall Shape : Rectangular Seats : 1’680 Voulme : 15’000 m3 Height : 17.4 m Length : 35.7 m Width : 19.8 m Reverberation t : 2.05s 10 V / ST : 13.4 m V / SA : 15.7 m V / N : 8.93 m3 SA / N : 0.57 m2 H / W : 0.88 L / W : 1.8 So : 163 m2 Sa : 690 m2 30 SA : 955 m2 ST : 1’118 m2 1-IACCE3 : 0.71 Decay time (EDT) : 2.2s Diffusivity (SDI) : 1.0 Loudness (G mid) : 5.5dB Intimacy (tI) : 12 msec Warmth (BR) : 1.11 105 1871 Royal Albert Hall London, Great Britain 0 Type : Concert hall Shape : Elliptic Seats : 5’080 + 1’000 Voulme : 86.650 m3 Height : 36 m Length : 44.5 m Width : 47 m Reverberation t : 2.4s 106 Appendix : Schemes 10 30 V / ST : 23.5 m V / SA : 24.7 m V / N : 17 m3 SA / N : 0.69 m2 H / W : 0.76 L / W : 0.94 So : 176 m2 Sa : 2’700 m2 SA : 3’512 m2 ST : 3’688 m2 1-IACCE3 : 0.52 Decay time (EDT) : 2.6s Diffusivity (SDI) : 0.5 Loudness (G mid) : -0.1dB Intimacy (tI) : 15 msec Warmth (BR) : 1.13 1875 Opéra Garnier Paris, France 0 Type : Theater Shape : Horseshoe Seats : 2’131 Voulme : 10’000 m3 Height : 20.7 m Length : 27.7 m Width : 18,9 ma Reverberation t : 1.15s 10 V / ST : 6.9 m V / SA : 8.87 m V / N : 4.68 m3 SA / N : 0.53 m2 H / W : 1.1 L / W : 1.47 So : 78 m2 Sa : 900 m2 30 SA : 1’126 m2 ST : 1’448 m2 1-IACCE3 : 0.50 Decay time (EDT) : 1.2s Diffusivity (SDI) : Loudness (G mid) : 1.2dB Intimacy (tI) : 17 msec Warmth (BR) : - 107 1876 Festspielhaus Bayreuth, Germany 0 Type : Theater Shape : Fan Seats : 1’800 Voulme : 10’308 m3 Height : 12.8 m Length : 32.3 m Width : 33.2 m Reverberation t : 1.55 108 Appendix : Schemes 10 30 V / ST : 10 m V / SA : 12.2 m V / N : 5.72 m3 SA / N : 0.47 m2 H / W : 0.385 L / W : 0.97 So : 34.5 m2 Sa : 755 m2 SA : 845 m2 ST : 1’032 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 14 msec Warmth (BR) : 1.11 1877 St. Andrew Hall Glasgow, Scotland 0 Type : Concert hall Shape : Rectangular Seats : 2’133 Voulme : 16’100 m3 Height : 22 m Length : 50 m Width : 14 m Reverberation t : 1.90s 10 V / ST : 11.6 m V / Sa : 12.8 m V / N : 7.6 m3 Sa / N : 0.59 m2 H / W : 1.57 L / W : 3.57 So : 130 m2 Sa : 1’255 m2 30 SA : ST : 1’385 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 109 1882 neues Gewandhaus Leipzig, Germany 0 Type : Concert hall Shape : Rectangular Seats : 1560 Voulme : 10’600 m3 Height : 14.9 m Length : 37.8 m Width : 18.9 m Reverberation t : 1.55s 110 Appendix : Schemes 10 30 V / ST : 10.3 m V / Sa :11.7 m V / N : 6.8 m3 Sa / N : 0.59 m2 H / W : 0.79 L / W : 2.0 So : 116 m2 Sa : 905 m2 SA : ST : 1’020 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1883 Metropolitan Opera House New York, USA 0 Type : Theater Shape : Horseshoe Seats : 3’816 Voulme : 24’724 m3 Height : 25 m Length : 39.6 m Width : 33.5 m Reverberation t : 1.8s 10 V / ST : 10.3 m V / SA : 10.9 m V / N : 6.48 m3 SA / N : 0.59 m2 H / W : 0.745 L / W : 1.18 So : 132 m2 Sa : 1’914 m2 30 SA : 2’262 m2 ST : 2’394 m2 1-IACCE3 : Decay time (EDT): 2.3s Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 34 msec Warmth (BR) : 1.20 111 1888 Concertgebouw Amsterdam, Netherlands 0 Type : Concert hall Shape : Rectangular Seats : 2’037 Voulme : 18’780 m3 Height : 17.1 m Length : 26.2 m Width : 27.7 m Reverberation t : 2.0s 112 Appendix : Schemes 10 30 V / ST : 14.6 m V / SA : 16.7 m V / N : 16.7 m3 SA / N : 0.55 m2 H / W : 0.62 L / W : 0.94 So : 160 m2 Sa : 843 m2 SA : 1’125 m2 ST : 1’285 m2 1-IACCE3 : 0.46 Decay time (EDT) : 2.2s Diffusivity (SDI) : 1.0 Loudness (G mid) : 5.9dB Intimacy (tI) : 21 msec Warmth (BR) : 1.08 1891a Carnegie Hall New York, USA 0 Type : Concert hall Shape : Horseshoe Seats : 2’804 Voulme : 24’270 m3 Height : 23.8 m Length : 32.9 m Width : 25.9 m Reverberation t : 1.8s 10 V / ST : 13.3 m V / SA : 15.2 m V / N : 8.65 m3 SA / N : 0.53 m2 H / W : 0.92 L / W : 1.27 So : 227 m2 Sa : 1’145 m2 30 SA : 1’600 m2 ST : 1’826 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 23 msec Warmth (BR) : - 113 1891b Orchestra Hall Chicago, USA 0 Type : Concert hall Shape : Horseshoe Seats : 2’582 Voulme : 18’000 m3 Height : 18 m Length : 25.6 m Width : 28.7 Reverberation t : 1.2s 114 Appendix : Schemes 10 30 V / ST : 9.7 m V / SA : 10.8 m V / N : 7.0 m3 SA / N : 0.65 m2 H / W : 0.63 L / W : 0.89 So : 186 m2 Sa : 1’290 m2 SA : 1’672 m2 ST : 1’858 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 36 msec Warmth (BR) : - 1894 Type : Concert hall Shape : Rectangular Seats : 1’644 Voulme : Height : Length : Width : Reverberation t : - Victoria Hall Geneva, Switzerland V / ST : V / SA : V / N : SA / N : H / W : L / W : So : Sa : - SA : ST : 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 115 1895 Grosser Tonhallesaal Zurich, Switzerland 0 Type : Concert hall Shape : Rectangular Seats : 1’546 Voulme : 11’400 m3 Height : 14 m Length : 29.6 m Width : 19.5 Reverberation t : 2.05s 116 Appendix : Schemes 10 30 V / ST : 11.2 m V / SA : 13 m V / N : 7.37 m3 SA / N : 0.57 m2 H / W : 0.72 L / W : 1.5 So : 145 m2 Sa : 702 m2 SA : 877 m2 ST : 1’022 m2 1-IACCE3 : 0.71 Decay time (EDT) : 2.2s Diffusivity (SDI) : 0.9 Loudness (G mid) : 6.7dB Intimacy (tI) : 14 msec Warmth (BR) : 1.23 1900 Symphony Hall Boston, USA 0 Type : Concert hall Shape : Rectangular Seats : 2’631 Voulme : 18’740 m3 Height : 18.6 m Length : 39 m Width : 23.6 m Reverberation t : 1.85s 10 V / ST : 12.3 m V / SA : 13.7 m V / N : 7.14 m3 SA / N : 0.52 m2 H / W : 0.81 L / W : 1.71 So : 152 m2 Sa : 1’056 m2 30 SA : 1’370 m2 ST : 1’550 m2 1-IACCE3 : 0.65 Decay time (EDT) : 2.1s Diffusivity (SDI) : 1.0 Loudness (G mid) : 4.7dB Intimacy (tI) : 15 msec Warmth (BR) : 1.03 117 1908 Teatro Colón Buenos Aires, Argentina 0 Type : Theater Shape : Horseshoe Seats : 2’787 Voulme : 20’570 m3 Height : 26.5 m Length : 34.4 m Width : 24.4 m Reverberation t : 1.8s 118 Appendix : Schemes 10 30 V / ST : 12.5 m V / SA : 15.4 m V / N : 8.01 m3 SA / N : 0.52 m2 H / W : 0.51 L / W : 1.1 So : 154 m2 Sa : 541 m2 SA : 701 m2 ST : 2’144 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 19 msec Warmth (BR) : - 1914 Usher Hall Edinburgh, Great Britain 0 Type : Concert hall Shape : Horseshoe Seats : 2’547 Voulme : 15’700 m3 Height : 17 m Length : 30.5 m Width : 23.8 m Reverberation t : 1.5s 10 V / ST : 10.8 m V / SA : 11.7 m V / N : 6.16 m3 SA / N : 0.525 m2 H / W : 0.72 L / W : 1.28 So : 120 m2 Sa : 1’040 m2 30 SA : 1’338 m2 ST : 1’458 m2 1-IACCE3 : Decay time (EDT) : 2.1s Diffusivity (SDI) : Loudness (G mid) : 4.6dB Intimacy (tI) : 33 msec Warmth (BR) : 1.17 119 1923 Eastman Theatre New York, USA 0 Type : Theater Shape : Fan Seats : 3’347 Voulme : 23’970 m3 Height : 20.4 m Length : 35.7 m Width : 36.6 m Reverberation t : 1.65s 120 Appendix : Schemes 10 30 V / ST : 10.2 m V / SA : 11.9 m V / N : 7.16 m3 SA / N : 0.60 m2 H / W : 0.56 L / W : 0.97 So : 204 m2 Sa : 1’580 m2 SA : 1’907 m2 ST : 2’348 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 55 msec Warmth (BR) : 1.26 1927 Salle Pléyel Paris, France 0 Type : Concert hall Shape : Fan Seats : 2’386 Voulme : 15’500 m3 Height : 18.6 m Length : 30.5 m Width : 25.6 m Reverberation t : 1.5s 10 V / ST : 11.9 m V / SA : 14.6 m V / N : 6.5 m3 SA / N : 0.44 m2 H / W : 0.73 L / W : 1.19 So : 242 m2 Sa : 780 m2 30 SA : 1’058 m2 ST : 1’300 m2 1-IACCE3 : 0.54 Decay time (EDT) : 1.8s Diffusivity (SDI) : 0.5 Loudness (G mid) : 4.5dB Intimacy (tI) : 35 msec Warmth (BR) : 1.23 121 1929 Palais des Beaux-Arts Brussels, Belgium 0 Type : Concert hall Shape : Elliptic Seats : 2’150 Voulme : 12’520 m3 Height : 29.3 m Length : 31.1 m Width : 23.2 m Reverberation t : 1.4s 122 Appendix : Schemes 10 30 V / ST : 8.42 m V / SA : 9.6 m V / N : 5.83 m3 SA / N : 0.60 m2 H / W : 1.26 L / W : 1.34 So : 186 m2 Sa : 1’020 m2 SA : 1’300 m2 ST : 1’486 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 23 msec Warmth (BR) : - 1930 War Memorial Opera House San Francisco, USA 0 Type : Theater Shape : Fan Seats : 3’252 Voulme : 20’900 m3 Height : 22.2 m Length : 36.6 m Width : 31.7 m Reverberation t : 1.5s 10 V / ST : 9.19 m V / SA : 10.6 m V / N : 6.43 m3 SA / N : 0.61 m2 H / W : 0.70 L / W : 1.15 So : 70.6 m2 Sa : 1’518 m2 30 SA : 1’973 m2 ST : 2’276 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 51 msec Warmth (BR) : - 123 1931 Severance Hall Cleveland, USA 0 Type : Concert hall Shape : Horseshoe Seats : 2’101 Voulme : 15’690 m3 Height : 16.8 m Length : 32.9 m Width : 27.4 m Reverberation t : 1.5s 124 Appendix : Schemes 10 30 V / ST : 11.2 m V / SA : 13 m V / N : 7.5 m3 SA / N : 0.57 m2 H / W : 0.61 L / W : 1.2 So : 186 m2 Sa : 930 m2 SA : 1’208 m2 ST : 1’394 m2 1-IACCE3 : 0.59 Decay time (EDT) : 1.7s Diffusivity (SDI) : 0.8 Loudness (G mid) : 3.9dB Intimacy (tI) : 20 msec Warmth (BR) : 1.14 1935 Konserthus Gothenburg, Sweden 0 Type : Concert hall Shape : Rectangular Seats : 1’286 Voulme : 11’900 m3 Height : 13.7 m Length : 30.5 m Width : 25.3 m Reverberation t : 1.65s 10 V / ST : 14.2 m V / SA : 17.8 m V / N : 9.25 m3 SA / N : 0.52 m2 H / W : 0.54 L / W : 1.2 So : 170 m2 Sa : 585 m2 30 SA : 666 m2 ST : 836 m2 1-IACCE3 : Decay time (EDT) : 1.8s Diffusivity (SDI) : Loudness (G mid) : 5.8dB Intimacy (tI) : 33 msec Warmth (BR) : 1.08 125 1938 Tanglewood, Serge Koussevitzky Music Shed Massachusetts, USA 0 Type : Concert hall Shape : Fan Seats : 5’121 Voulme : 42’480 m3 Height : 13.4 m Length : 50.9 m Width : 61 m Reverberation t : 1.9s 126 Appendix : Schemes 10 30 V / ST : 13.9 m V / SA : 14.8 m V / N : 8.29 m3 SA / N : 0.56 m2 H / W : 0.22 L / W : 0.835 So : 204 m2 Sa : 2’200 m2 SA : 2’861 m2 ST : 3’065 m2 1-IACCE3 : 0.46 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.8 Loudness (G mid) : 4.9dB Intimacy (tI) : 19 msec Warmth (BR) : 1.45 1939 Philharmonic Hall Liverpool, Great Britain 0 Type : Concert hall Shape : Fan Seats : 1’824 Voulme : 13’560 m3 Height : 14 m Length : 28.6 m Width : 30 m Reverberation t : 1.5s 10 V / ST : 9.54 m V / SA : 10.5 m V / N : 7.43 m3 SA / N : 0.71 m2 H / W : 0.47 L / W : 0.96 So : 130 m2 Sa : 994 m2 30 SA : 1’291 m2 ST : 1’421 m2 1-IACCE3 : 0.6 Decay time (EDT) : 1.8s Diffusivity (SDI) : 0.4 Loudness (G mid) : 3.9dB Intimacy (tI) : 25 msec Warmth (BR) : 1.00 127 1940 Kleinhans Music Hall Buffalo, USA 0 Type : Concert hall Shape : Fan Seats : 2’839 Voulme : 18’240 m3 Height : 13.4 m Length : 37.5 m Width : 39.3 m Reverberation t : 1.3s 128 Appendix : Schemes 10 30 V / ST : 8.5 m V / SA : 9.35 m V / N : 6.42 m3 SA / N : 0.69 m2 H / W : 0.34 L / W : 0.95 So : 205 m2 Sa : 1’580 m2 SA : 1’951 m2 ST : 2’156 m2 1-IACCE3 : 0.41 Decay time (EDT) : 1.6s Diffusivity (SDI) : 0.3 Loudness (G mid) : 2.9dB Intimacy (tI) : 32 msec Warmth (BR) : 1.28 1945 Radiohuset, Studio 1 Copenhagen, Denmark 0 Type : Concert hall Shape : Fan Seats : 1’081 Voulme : 11’900 m3 Height : 17.7 m Length : 18.6 m Width : 33.5 m Reverberation t : 1.5s 10 V / ST : 11.8 m V / SA : 16.5 m V / N : 11 m3 SA / N : 0.67 m2 H / W : 0.53 L / W : 0.55 So : 288 m2 Sa : 605 m2 30 SA : 721 m2 ST : 1’009 m2 1-IACCE3 : 0.58 Decay time (EDT) : 2.0s Diffusivity (SDI) : 0.5 Loudness (G mid) : 6.4dB Intimacy (tI) : 29 msec Warmth (BR) : 1.07 129 1951a Colston Hall Bristol, Great Britain 0 Type : Concert hall Shape : Rectangular Seats : 2’121 Voulme : 13’450 m3 Height : 17.7 m Length : 27.4 m Width : 22.6 m Reverberation t : 1.85s 130 Appendix : Schemes 10 30 V / ST : 11.7 m V / SA : 13.6 m V / N : 6.34 m3 SA / N : 0.47 m2 H / W : 0.78 L / W : 1.21 So : 160 m2 Sa : 745 m2 SA : 987 m2 ST : 1’147 m2 1-IACCE3 : 0.63 Decay time (EDT): 1.9s Diffusivity (SDI) : 0.3 Loudness (G mid) : 5.8dB Intimacy (tI) : 21 msec Warmth (BR) : 1.05 1951b Free Trade Hall Manchester, Great Britain 0 Type : Concert hall Shape : Rectangular Seats : 2’351 Voulme : 15’430 m3 Height : 20.7 m Length : 28 m Width : 24.4 m Reverberation t : 1.6s 10 V / ST : 9.92 m V / SA : 11.2 m V / N : 6.6 m3 SA / N : 0.58 m2 H / W : 0.85 L / W : 1.15 So : 100 m2 Sa : 1’057 m2 30 SA : 1’375 m2 ST : 1’555 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : 4.1dB Intimacy (tI) : 25 msec Warmth (BR) : 0.97 131 1951c Royal Festival Hall London, Great Britain 0 Type : Concert hall Shape : Rectangular Seats : 2’901 Voulme : 21’950 m3 Height : 15.2 m Length : 36.8 m Width : 32.3 m Reverberation t : 1.5s 132 Appendix : Schemes 10 30 V / ST : 10.2 m V / SA : 11.1 m V / N : 7.56 m3 SA / N : 0.68 m2 H / W : 0.47 L / W : 1.14 So : 173 m2 Sa : 1’540 m2 SA : 1’972 m2 ST : 2’145 m2 1-IACCE3 : 0.63 Decay time (EDT) : 1.7s Diffusivity (SDI) : 0.6 Loudness (G mid) : 2.6dB Intimacy (tI) : 34 msec Warmth (BR) : 1.17 1953 Herkulessaal Munich, Germany 0 Type : Concert hall Shape : Rectangular Seats : 1’287 Voulme : 13’590 m3 Height : 15.5 m Length : 32 m Width : 22 m Reverberation t : 1.8s 10 V / ST : 16.1 m V / SA : 20.2 m V / N : 10.6 m3 SA / N : 0.52 m2 H / W : 0.71 L / W : 1.46 So : 168 m2 Sa : 585.7 m2 30 SA : 674 m2 ST : 842 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 24 msec Warmth (BR) : - 133 1954a Musikhochschule Konzertsaal Berlin, Germany 0 Type : Concert Hall Shape : Diamond Seats : 1’032 Voulme : 9’600 m3 Height : 15 m Length : 32 m Width : 20 m Reverberation t : 1.65s 134 Appendix : Schemes 10 30 V / ST : 10.5 m V / Sa : 13.0 m V / N : 7.6 m3 Sa / N : 0.56 m2 H / W : 0.75 L / W : 1.6 So : 170 m2 Sa : 740 m2 SA : ST : 910 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1954b Aula Magna Caracas, Venezuela 0 Type : Concert Hall Shape : Fan Seats : 2’660 Voulme : 24’920 m3 Height : 17.7 m Length : 31.1 m Width : 57.6 m Reverberation t : 1.7s 10 V / ST : 11.9 m V / SA : 13.2 m V / N : 9.37 m3 SA / N : 0.71 m2 H / W : 0.31 L / W : 0.54 So : 204 m2 Sa : 1’580 m2 30 SA : 1’886 m2 ST : 2’090 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 30 msec Warmth (BR) : - 135 1955a Salle Musica La Chaux-de-Fonds, Switzerland 0 Type : Concert Hall Shape : Rectangular Seats : 1’032 Voulme : 7’780 m3 Height : 14 m Length : 26.5 m Width : 21 m Reverberation t : 1.7s 136 Appendix : Schemes 10 30 V / ST : 10.0 m V / Sa : 12.0 m V / N : 7.5 m3 Sa / N : 0.63 m2 H / W : 0.67 L / W : 1.26 So : 125 m2 Sa : 650 m2 SA : ST : 775 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : Warmth (BR) : - 1955b Academy of Music Philadelphia, USA 0 Type : Theater Shape : Horseshoe Seats : 2’827 Voulme : 15’100 m3 Height : 19.5 m Length : 31.1 m Width : 17.7 m Reverberation t : 1.2s 10 V / ST : 8.7 m V / SA : 10.4 m V / N : 5.38 m3 SA / N : 0.52 m2 H / W : 1.1 L / W : 1.76 So : 59 m2 Sa : 1’300 m2 30 SA : 1’460 m2 ST : 1’740 m2 1-IACCE3 : 0.47 Decay time (EDT) : 1.2s Diffusivity (SDI) : Loudness (G mid) : 2.0dB Intimacy (tI) : 19 msec Warmth (BR) : 1.12 137 1955c Staatsoper Vienna, Austria 0 Type : Theater Shape : Horseshoe Seats : 1’709 Voulme : 10’665 m3 Height : 18.9 m Length : 29.9 m Width : 18.3 m Reverberation t : 1.3s 138 Appendix : Schemes 10 30 V / ST : 7.3 m V / SA : 8.9 m V / N : 6.24 m3 SA / N : 0.72 m2 H / W : 1.03 L / W : 1.63 So : 106.8 m2 Sa : 930 m2 SA : 1’194 m2 ST : 1’460 m2 1-IACCE3 : 0.60 Decay time (EDT) : 1.4s Diffusivity (SDI) : Loudness (G mid) : 2.2dB Intimacy (tI) : 15 msec Warmth (BR) : 1.10 1956a Neue Liederhalle Stuttgart, Germany 0 Type : Concert Hall Shape : asymmetric Seats : 2’000 Voulme : 16’000 m3 Height : 13.4 m Length : 41.8 m Width : 36.2 m Reverberation t : 1.6s 10 V / ST : 10.4 m V / SA : 12.3 m V / N : 8.0 m3 SA / N : 0.65 m2 H / W : 0.37 L / W : 1.15 So : 176 m2 Sa : 1’000 m2 30 SA : 1’300 m2 ST : 1’533 m2 1-IACCE3 : 0.44 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.5 Loudness (G mid) : 4.3dB Intimacy (tI) : 29 msec Warmth (BR) : 1.00 139 1956b Tivoli Koncertsal Copenhagen, Denmark 0 Type : Theater Shape : Fan Seats : 1’789 Voulme : 12’740 m3 Height : 13.7 m Length : 32.3 m Width : 33.2 m Reverberation t : 1.3s 140 Appendix : Schemes 10 V / ST : 9.6 m V / SA : 11.2 m V / N : m3 SA / N : m2 H / W : 0.41 L / W : 0.97 So : 195 m2 Sa : 988 m2 30 SA : 1’136 m2 ST : 1’331 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 16 msec Warmth (BR) : - 1957a Kulttuuritalo Helsinki, Finland 0 Type : Concert Hall Shape : Asymmetric Seats : 1’500 Voulme : 10’025 m3 Height : 9.45 m Length : 23.8 m Width : 46 m Reverberation t : 1.05s 10 V / ST : 9 m V / SA : 10.6 m V / N : 6.7 m3 SA / N : 0.63 m2 H / W : 0.2 L / W : 0.52 So : 166 m2 Sa : 860 m2 30 SA : 946 m2 ST : 1’112 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 26 msec Warmth (BR) : - 141 1957b Frederic R. Mann Auditorium Tel Aviv, Isreal 0 Type : Concert Hall Shape : Fan Seats : 2’715 Voulme : 21’240 m3 Height : 12.2 m Length : 30.5 m Width : 40.2 m Reverberation t : 1.55s 142 Appendix : Schemes 10 30 V / ST : 11 m V / SA : 12.5 m V / N : 6.76 m3 SA / N : 0.54 m2 H / W : 0.30 L / W : 0.76 So : 195 m2 Sa : 1’350 m2 SA : 1’700 m2 ST : 1’932 m2 1-IACCE3 : 0.41 Decay time (EDT) : 1.7s Diffusivity (SDI) : 0.5 Loudness (G mid) : 2.9dB Intimacy (tI) : 30 msec Warmth (BR) : 0.98 1957c Northern Alberta Jubilee Auditorium Edmonton, Canada 0 Type : Concert Hall Shape : Fan Seats : 2’678 Voulme : 21’500 m3 Height : 15.8 m Length : 40 m Width : 34.8 m Reverberation t : 1.4s 10 V / ST : 10 m V / SA : 11 m V / N : 8.0 m3 SA / N : 0.73 m2 H / W : 0.46 L / W : 1.15 So : 186 m2 Sa : 1’500 m2 30 SA : 1’951 m2 ST : 2’137 m2 1-IACCE3 : 0.49 Decay time (EDT) : 1.4s Diffusivity (SDI) : 0.3 Loudness (G mid) : 0.4dB Intimacy (tI) : 31 msec Warmth (BR) : 0.99 143 1959 Beethovenhalle Bonn, Germany 0 Type : Concert Hall Shape : Asymmetric Seats : 1’407 Voulme : 15’728 m3 Height : 12.2 m Length : 34.8 m Width : 36.6 m Reverberation t : 1.65s 144 Appendix : Schemes 10 30 V / ST : 11.9 m V / SA : 14.1 m V / N : 11.2 m3 SA / N : 0.79 m2 H / W : 0.33 L / W : 0.95 So : 204 m2 Sa : 864 m2 SA : 1’115 m2 ST : 1’320 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 27 msec Warmth (BR) : - 1960a Festspielhaus Salzburg, Austria 0 Type : Theater Shape : Fan Seats : 2’158 Voulme : 14’020 m3 Height : 14.3 m Length : 29.6 m Width : 32.9 m Reverberation t : 1.5s 10 V / ST : 9.9 m V / SA : 11.3 m V / N : 7.2 m3 SA / N : 0.30 m2 H / W : 0.44 L / W : 0.9 So : 195 m2 Sa : 1’058 m2 30 SA : 1’375 m2 ST : 1’570 m2 1-IACCE3 : Decay time (EDT) : 1.9s Diffusivity (SDI) : Loudness (G mid) : 4.0dB Intimacy (tI) : 23 msec Warmth (BR) : 1.10 145 1960b Binyanei Ha’Oomah Jerusalem, Israel 0 Type : Concert Hall Shape : Fan Seats : 3’142 Voulme : 24’700 m3 Height : 13.7 m Length : 37.2 m Width : 47.6 m Reverberation t : 1.75s 146 Appendix : Schemes 10 30 V / ST : 10.3 m V / SA : 11.6 m V / N : 7.9 m3 SA / N : 0.68 m2 H / W : 0.29 L / W : 0.78 So : 260 m2 Sa : 1’672 m2 SA : 2’137 m2 ST : 2’400 m2 1-IACCE3 : 0.55 Decay time (EDT) : 1.9s Diffusivity (SDI) : 0.4 Loudness (G mid) : 2.6dB Intimacy (tI) : 26 msec Warmth (BR) : 1.05 1962 Avery Fisher Hall New York, USA 0 Type : Concert Hall Shape : Rectangular Seats : 2’742 Voulme : 20’400 m3 Height : 16.8 m Length : 38.4 m Width : 25.9 m Reverberation t : 1.75s 10 V / ST : 12.1 m V / SA : 13.8 m V / N : 7.44 m3 SA / N : 0.54 m2 H / W : 0.65 L / W : 1.5 So : 203 m2 Sa : 1’189 m2 30 SA : 1’480 m2 ST : 1’683 m2 1-IACCE3 : 0.54 Decay time (EDT) : 2.0s Diffusivity (SDI) : 0.7 Loudness (G mid) : 3.8dB Intimacy (tI) : 30 msec Warmth (BR) : 0.93 147 1963 Berlin Philharmonie Berlin, Germany 0 Type : Concert Hall Shape : Freeform Seats : 2’215 + 120 Voulme : 21’000 m3 Height : 12.8 m Length : 29 m Width : 42.7 m Reverberation t : 1.95s 148 Appendix : Schemes 10 30 V / ST : 13.5 m V / SA : 15.2 m V / N : 9 m3 SA / N : 0.62 m2 H / W : 0.3 L / W : 0.68 So : 172.5 m2 Sa : 1’057 m2 SA : 1’385 m2 ST : 1’558 m2 1-IACCE3 : 0.46 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.8 Loudness (G mid) : 4.3dB Intimacy (tI) : 21 msec Warmth (BR) : 1.01 1966 De Doelen Concertgebouw Rotterdam, Netherlands 0 Type : Concert Hall Shape : Diamond Seats : 2’242 Voulme : 24’070 m3 Height : 14.3 m Length : 31.7 m Width : 32.3 m Reverberation t : 2.0s 10 V / ST : 14.2 m V / SA : 16 m V / N : 10.7 m3 SA / N : 0.67 m2 H / W : 0.44 L / W : 0.98 So : 195 m2 Sa : 1’051 m2 30 SA : 1’509 m2 ST : 1’704 m2 1-IACCE3 : 0.55 Decay time (EDT) : 2.3s Diffusivity (SDI) : 0.9 Loudness (G mid) : 3.2dB Intimacy (tI) : 35 msec Warmth (BR) : 0.95 149 1972 Christenchurch Town Hall Christenchurch, New Zealand 0 Type : Concert Hall Shape : Elliptic Seats : 2’662 Voulme : 20’500 m3 Height : 18.6 m Length : 28 m Width : 29.3 m Reverberation t : 1.9s 150 Appendix : Schemes 10 30 V / ST : 12.7 m V / SA : 14.5 m V / N : 7.7 m3 SA / N : 0.53 m2 H / W : 0.64 L / W : 0.96 So : 194 m2 Sa : 1’127 m2 SA : 1’416 m2 ST : 1’610 m2 1-IACCE3 : 0.55 Decay time (EDT) : 2.0s Diffusivity (SDI) : 0.6 Loudness (G mid) : 3.8dB Intimacy (tI) : 11 msec Warmth (BR) : 1.06 1973a Sydney Opera House Sydney, Australia 0 Type : Concert Hall Shape : Diamond Seats : 2’679 Voulme : 24’600 m3 Height : 16.8 m Length : 31.7 m Width : 33.2 m Reverberation t : 2.0s 10 V / ST : 14.0 m V / SA : 15.7 m V / N : 9.18 m3 SA / N : 0.58 m2 H / W : 0.50 L / W : 0.95 So : 180.7 m2 Sa : 1’362 m2 30 SA : 1’563 m2 ST : 1’744 m2 1-IACCE3 : Decay time (EDT) : 2.2s Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 36 msec Warmth (BR) : - 151 1973b NHK Hall Tokyo, Japan 0 Type : Concert Hall Shape : Fan Seats : 3’677 Voulme : 25’200 m3 Height : 14.9 m Length : 37.8 m Width : 38.4 m Reverberation t : 1.7s 152 Appendix : Schemes 10 V / ST : 12.5 m V / SA : 13.8 m V / N : 6.85 m3 SA / N : 0.5 m2 H / W : 0.39 L / W : 0.87 So : 193 m2 Sa : 1’458 m2 30 SA : 1’821 m2 ST : 2’014 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 23 msec Warmth (BR) : - 1974 Minnesota Orchestra Hall Minneapolis, USA 0 Type : Concert Hall Shape : Rectangular Seats : 2’450 Voulme : 18’975 m3 Height : 16.5 m Length : 38.1 m Width : 40.8 m Reverberation t : 1.8s 10 V / ST : 10.7 m V / SA : 12 m V / N : 7.74 m3 SA / N : 0.64 m2 H / W : 0.57 L / W : 1.33 So : 203 m2 Sa : 1’266 m2 30 SA : 1’574 m2 ST : 1’777 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 33 msec Warmth (BR) : - 153 1975 Bunka Kaikan Tokyo, Japan 0 Type : Concert Hall Shape : Diamond Seats : 2’327 Voulme : 17’300 m3 Height : 17.4 m Length : 31.7 m Width : 26.5 m Reverberation t : 1.5s 154 Appendix : Schemes 10 30 V / ST : 11.2 m V / SA : 13.3 m V / N : 7.4 m3 SA / N : 0.56 m2 H / W : 0.66 L / W : 1.2 So : 241 m2 Sa : 983 m2 SA : 1’301 m2 ST : 1’542 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 14msec Warmth (BR) : - 1976 Sala Nezahualcoyotl Mexico City, Mexico 0 Type : Concert Hall Shape : Fan Seats : 2’376 Voulme : 30’640 m3 Height : 15.8 m Length : 34.4 m Width : 40.8 m Reverberation t : 1.9s 10 V / ST : 15.7 m V / SA : 18.2 m V / N : 12.9 m3 SA / N : 0.71 m2 H / W : 0.39 L / W : 0.84 So : 270 m2 Sa : 1’476 m2 30 SA : 1’684 m2 ST : 1’954 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 16 msec Warmth (BR) : - 155 1979 Abravanel Symphony Hall Salt Lake City, USA 0 Type : Concert Hall Shape : Rectangular Seats : 2’812 Voulme : 19’500 m3 Height : 16.5 m Length : 37.8 m Width : 29.3 m Reverberation t : 1.7s 156 Appendix : Schemes 10 30 V / ST : 10.3 m V / SA : 11.7 m V / N : 6.93 m3 SA / N : 0.59 m2 H / W : 0.56 L / W : 1.29 So : 218 m2 Sa : 1’486 m2 SA : 1’669m2 ST : 1’887 m2 1-IACCE3 : 0.59 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.6 Loudness (G mid) : 2.0dB Intimacy (tI) : 30 msec Warmth (BR) : 1.06 1981 Gewandhaus Leipzig, Germany 0 Type : Concert Hall Shape : Fan Seats : 1’900 Voulme : 21’000 m3 Height : 19.8 m Length : 32.3 m Width : 36 m Reverberation t : 2.0s 10 V / ST : 15.2 m V / SA : 17.6 m V / N : 11 m3 SA / N : 0.63 m2 H / W : 0.55 L / W : 0.90 So : 181 m2 Sa : 1’036 m2 30 SA : 1’197m2 ST : 1’378 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 27 msec Warmth (BR) : - 157 1982a Barbican Hall London, Great Britain 0 Type : Concert Hall Shape : Fan Seats : 2’026 Voulme : 17’750 m3 Height : 14.3 m Length : 27.4 m Width : 39.3 m Reverberation t : 1.65s 158 Appendix : Schemes 10 30 V / ST : 11.9 m V / SA : 13.4 m V / N : 8.76 m3 SA / N : 0.65 m2 H / W : 0.36 L / W : 0.70 So : 160 m2 Sa : 1’123 m2 SA : 1’326 m2 ST : 1’485 m2 1-IACCE3 : 0.46 Decay time (EDT) : 1.9s Diffusivity (SDI) : 0.3 Loudness (G mid) : 3.4dB Intimacy (tI) : 27 msec Warmth (BR) : 1.07 1982b Joseph Meyerhoff Symphony Hall Baltimore, USA 0 Type : Concert Hall Shape : Elliptic Seats : 2’467 Voulme : 21’524 m3 Height : 18 m Length : 35.4 m Width : 29.3 m Reverberation t : 2.0s 10 V / ST : 12.9 m V / SA : 14.5 m V / N : 8.72 m3 SA / N : 0.60 m2 H / W : 0.61 L / W : 1.21 So : 186 m2 Sa : 1’196 m2 30 SA : 1’486 m2 ST : 1’672 m2 1-IACCE3 : 0.54 Decay time (EDT) : 2.3s Diffusivity (SDI) : 0.8 Loudness (G mid) : 4.1dB Intimacy (tI) : 13 msec Warmth (BR) : 1.10 159 1982c Roy Thompson Hall Toronto, Canada 0 Type : Concert Hall Shape : Elliptic Seats : 2’812 Voulme : 28’300 m3 Height : 23.2 m Length : 27.1 m Width : 31.1 m Reverberation t : 1.8s 160 Appendix : Schemes 10 30 V / ST : 14.9 m V / SA : 16.8 m V / N : 10.1 m3 SA / N : 0.60 m2 H / W : 0.74 L / W : 0.87 So : 222 m2 Sa : 1’401 m2 SA : 1’681 m2 ST : 1’903 m2 1-IACCE3 : 0.54 Decay time (EDT) : 1.9s Diffusivity (SDI) : 0.5 Loudness (G mid) : 3.8dB Intimacy (tI) : 35 msec Warmth (BR) : 1.10 1982d St. David’s Hall Wales, Great Britain 0 Type : Concert Hall Shape : Fan Seats : 1’952 Voulme : 22’000m3 Height : 18 m Length : 27.4 m Width : 27.4 m Reverberation t : 2.0s 10 V / ST : 15.5 m V / SA : 17.8 m V / N : 11.2 m3 SA / N : 0.63 m2 H / W : 0.66 L / W : 1.0 So : 186 m2 Sa : 1’000 m2 30 SA : 1’235 m2 ST : 1’420 m2 1-IACCE3 : 0.60 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.6 Loudness (G mid) : 3.8dB Intimacy (tI) : 25 msec Warmth (BR) : 0.96 161 1982e Symphony Hall Osaka, Japan 0 Type : Concert Hall Shape : Rectangular Seats : 1’702 Voulme : 17’800 m3 Height : 20.7 m Length : 28.3 m Width : 31.7 m Reverberation t : 2.0s 162 Appendix : Schemes 10 30 V / ST : 11.7 m V / SA : 14.4 m V / N : 10.5 m3 SA / N : 0.725 m2 H / W : 0.65 L / W : 0.89 So : 285 m2 Sa : 908 m2 SA : 1’236 m2 ST : 1’521 m2 1-IACCE3 : 0.56 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.8 Loudness (G mid) : 4.6dB Intimacy (tI) : 35 msec Warmth (BR) : 1.00 1985a Pátria Hall Budapest, Hungary 0 Type : Concert Hall Shape : Fan Seats : 1’750 Voulme : 13’400 m3 Height : 13.1 m Length : 26.2 m Width : 42.1 m Reverberation t : 1.6s 10 V / ST : 9.3 m V / SA : 10.4 m V / N : 7.66 m3 SA / N : 0.73 m2 H / W : 0.31 L / W : 0.62 So : 156 m2 Sa : 1’140 m2 30 SA : 1’286 m2 ST : 1’442 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 44 msec Warmth (BR) : - 163 1985b Philharmonie am Gasteig Munich, Germany 0 Type : Concert Hall Shape : Asymmetric Seats : 2’387 + 100 Voulme : 29’737 m3 Height : 14.6 m Length : 40.8 m Width : 51.2 m Reverberation t : 1.95s 164 Appendix : Schemes 10 30 V / ST : 15.9 m V / SA : 18.1 m V / N : 12.4 m3 SA / N : 0.69 m2 H / W : 0.29 L / W : 0.80 So : 230 m2 Sa : 1’329 m2 SA : 1’639 m2 ST : 1’869 m2 1-IACCE3 : 0.49 Decay time (EDT) : 2.1s Diffusivity (SDI) : 0.8 Loudness (G mid) : 2.2dB Intimacy (tI) : 29 msec Warmth (BR) : 1.00 1986a Suntory Tokyo, Japan 0 Type : Concert Hall Shape : Rectangular Seats : 2’006 Voulme : 21’000 m3 Height : 16.5 m Length : 30.5 m Width : 31.1 m Reverberation t : 2.0s 10 V / ST : 13.1 m V / SA : 15.4 m V / N : 10.5 m3 SA / N : 0.68 m2 H / W : 0.53 L / W : 0.98 So : 235 m2 Sa : 1’042 m2 30 SA : 1’364 m2 ST : 1’600 m2 1-IACCE3 : 0.53 Decay time (EDT) : 2.3s Diffusivity (SDI) : Loudness (G mid) : 4.6dB Intimacy (tI) : 30 msec Warmth (BR) : - 165 1986b Segerstrom Hall California, USA 0 Type : Concert Hall Shape : Asymmetric Seats : 2’903 Voulme : 27’800 m3 Height : 24.4 m Length : 36.2 m Width : 41.5 m Reverberation t : 1.6s 166 Appendix : Schemes 10 V / ST : 14.2 m V / SA : 18.5 m V / N : 9.58 m3 SA / N : 0.6 m2 H / W : 0.59 L / W : 0.88 So : 223 m2 Sa : 1’504 m2 30 SA : 1’742 m2 ST : 1’965 m2 1-IACCE3 : 0.62 Decay time (EDT) : 2.2s Diffusivity (SDI) : 0.9 Loudness (G mid) : 4.4dB Intimacy (tI) : 31 msec Warmth (BR) : 1.32 1987a Cultural Centre Concert Hall Taipei, Taiwan 0 Type : Concert Hall Shape : Rectangular Seats : 2’074 Voulme : 16’700 m3 Height : 18 m Length : 26.8 m Width : 32.3 m Reverberation t : 2.0s 10 V / ST : 10.9 m V / SA : 13.2 m V / N : 8 m3 SA / N : 0.61 m2 H / W : 0.67 L / W : 1.2 So : 269 m2 Sa : 1’022 m2 30 SA : 1’261 m2 ST : 1’530 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 29 msec Warmth (BR) : - 167 1987b Kammermusiksaal der Philharmonie Berlin, Germany 0 Type : Concert Hall Shape : Freeform Seats : 1’138 Voulme : 11’000m3 Height : 11.3 m Length : 18.3 m Width : 48.5m Reverberation t : 1.8s 168 Appendix : Schemes 10 30 V / ST : 12.1 m V / SA : 13.6 m V / N : 9.66 m3 SA / N : 0.71 m2 H / W : 0.23 L / W : 0.38 So : 78.2 m2 Sa : 618 m2 SA : 810 m2 ST : 907 m2 1-IACCE3 : Decay time (EDT) : 2.0s Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 20 msec Warmth (BR) : - 1989a Eugene McDermott Concert Hall Dallas, USA 0 Type : Concert Hall Shape : Horseshoe Seats : 2’065 Voulme : 23’900 m3 Height : 26.2 m Length : 30.8 m Width : 25.6 m Reverberation t : 2.0s 10 V / ST : 16.4 m V / SA : 20.6 m V / N : 11.6 m3 SA / N : 0.56 m2 H / W : 1.02 L / W : 1.2 So : 250 m2 Sa : 980 m2 30 SA : 1’161 m2 ST : 1’460 m2 1-IACCE3 : Decay time (EDT) : 2.0s Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 21 msec Warmth (BR) : - 169 1989b Orchard Hall Tokyo, Japan 0 Type : Concert Hall Shape : Fan Seats : 2’150 Voulme : 20’500m3 Height : 23 m Length : 38.4 m Width : 24.4 m Reverberation t : 1.8s 170 Appendix : Schemes 10 30 V / ST : 13.4 m V / SA : 15.6 m V / N : 9.53 m3 SA / N : 0.61 m2 H / W : 0.94 L / W : 1.57 So : 217 m2 Sa : 1’000 m2 SA : 1’314 m2 ST : 1’531 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 26 msec Warmth (BR) : - 1989c Opéra Bastille Paris, France 0 Type : Theater Shape : Elliptic Seats : 2’700 Voulme : 21’000 m3 Height : 21.3 m Length : 31.1 m Width : 16.2 m Reverberation t : 1.55 s 10 V / ST : 10.8 m V / SA : 13.8 m V / N : 7.8 m3 SA / N : 0.56 m2 H / W : 0.66 L / W : 1.16 So : 186 m2 Sa : 1’286 m2 30 SA : 1’522 m2 ST : 1’951 m2 1-IACCE3 : Decay time (EDT) : 1.6s Diffusivity (SDI) : Loudness (G mid) : 2.0dB Intimacy (tI) : 41 msec Warmth (BR) : 1.05 171 1990a Metropolitan Art Space Tokyo, Japan 0 Type : Concert Hall Shape : Fan Seats : 2’017 Voulme : 25’000 m3 Height : 15.5 m Length : 35 m Width : 28 m Reverberation t : 2.15s 172 Appendix : Schemes 10 30 V / ST : 16.5 m V / SA : 19 m V / N : 12.4 m3 SA / N : 0.65 m2 H / W : 0.55 L / W : 1.25 So : 207 m2 Sa : 929 m2 SA : 1’312 m2 ST : 1’519 m2 1-IACCE3 : 0.48 Decay time (EDT) : 2.6s Diffusivity (SDI) : Loudness (G mid) : 4.0dB Intimacy (tI) : 27 msec Warmth (BR) : - 1990b Royal Concert Hall Glasgow, Great Britain 0 Type : Concert Hall Shape : Rectangular Seats : 2’459 Voulme : 22’700 m3 Height : 19.2 m Length : 27.8 m Width : 32.9 m Reverberation t : 1.75s 10 V / ST : 14.3 m V / SA : 16.6 m V / N : 9.23 m3 SA / N : 0.56 m2 H / W : 0.58 L / W : 0.83 So : 218 m2 Sa : 1’074 m2 30 SA : 1’365 m2 ST : 1’584 m2 1-IACCE3 : 0.77 Decay time (EDT) : 1.7s Diffusivity (SDI) : 0.8 Loudness (G mid) : 2.2dB Intimacy (tI) : 20 msec Warmth (BR) : 1.12 173 1991 Symphony Hall Birmingham, Great Britain 0 Type : Concert Hall Shape : Horseshoe Seats : 2’211 Voulme : 25’000 m3 Height : 22.9 m Length : 31.7 m Width : 27.4 m Reverberation t : 1.85s 174 Appendix : Schemes 10 30 V / ST : 15.6 m V / SA : 18.9 m V / N : 11.3 m3 SA / N : 0.60 m2 H / W : 0.83 L / W : 1.15 So : 279 m2 Sa : 1’031 m2 SA : 1’320 m2 ST : 1’599 m2 1-IACCE3 : Decay time (EDT) : 2.0s Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 27 msec Warmth (BR) : - 1992 Hamarikyu Asahi Hall Tokyo, Japan 0 Type : Concert Hall Shape : Rectangular Seats : 552 Voulme : 5’800 m3 Height : 12 m Length : 24.7 m Width : 15 m Reverberation t : 1.7s 10 V / ST : 11.4 m V / SA : 13.3 m V / N : 10.5 m3 SA / N : 0.79 m2 H / W : 0.8 L / W : 1.65 So : 73 m2 Sa : 283 m2 30 SA : 395 m2 ST : 468 m2 1-IACCE3 : 0.40 Decay time (EDT) : 1.8s Diffusivity (SDI) : Loudness (G mid) : 9.8dB Intimacy (tI) : 16 msec Warmth (BR) : - 175 1994 Seiji Ozawa Hall Massachussets, USA 0 Type : Concert Hall Shape : Rectangular Seats : 1’180 Voulme : 11’610 m3 Height : 14.9 m Length : 28.6 m Width : 20.7 m Reverberation t : 1.7s 176 Appendix : Schemes 10 30 V / ST : 12.3 m V / SA : 15.7 m V / N : 9.83 m3 SA / N : 0.63 m2 H / W : 0.72 L / W : 1.38 So : 202 m2 Sa : 496 m2 SA : 739 m2 ST : 941 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 23 msec Warmth (BR) : 1.32 1999 Indiana University Auditorium Bloomington, USA 0 Type : Theater Shape : Fan Seats : 3’718 Voulme : 25’545 m3 Height : 13.7 m Length : 52.7 m Width : 39.3 m Reverberation t : 1.4s 10 V / ST : 9.72 m V / SA : 10.7 m V / N : 6.9 m3 SA / N : 0.64 m2 H / W : 0.35 L / W : 1.34 So : 81.6 m2 Sa : 1’915 m2 30 SA : 2’391 m2 ST : 2’626 m2 1-IACCE3 : Decay time (EDT) : Diffusivity (SDI) : Loudness (G mid) : Intimacy (tI) : 40 msec Warmth (BR) : 1.12 177 references REFERENCES • ADAM, Max, Raum und Bauakustik, Blauen, Schweizer Baudokumentation, 1985. • ANDO & NOSON, Ando & Dennis, Music & Concert Hall Acoustics, London, Academic Press, 1997. • ANDO, Yoichi, Architectural Acoustics - Blending Sound Sources, Sound Fields and Listeners, USA, Springers-Verlag New York Inc., 1998. • ANDO, Yoichi, Concert Hall Acoustics and Opera House Acoustics, in: Journal of sound and vibration vol. 258 no. 3, Elsevier Science, 2002. • BARRON, Michael, Auditorium Acoustics and Architectural Design, England, E & FN Spon, 1993. • BERANEK, Leo, Concert and Opera Halls - How they sound, USA, Acoustical Society of America, 1996. • BERANEK, Leo, Concert Halls and Opera Houses, USA, Springer-Verlag New York, 2004. • BOYER, Guy, La salle Pleyel, Lausanne, connaissance des arts, 2006. • CAVANAUGH & WILKES, William & Joseph, Architectural Acoustics - principles and practice, USA, John Wiley & Sons Inc., 1999. • CLASIEN, Delphine, Une salle de concert à Maastricht, Lausanne, Projet de Master EPFL, 1997. • FORSYTH, Michael, Architecture et musique, Belgium, Pierre Mardaga, 1985. • GRUENEISEN, Peter, Soundspace, Berlin, Birkhäuser, 2003. • HAMAYON, Loïc, Réussir l’acoustique d’un bâtiment, Paris, Groupe Moniteur, 2006. • KADEN, Christian, Das Unerhörte und das Unerhörbare, Kassel, Bärenreiter Verlag, 2004. • LONG, Marshall, Architectural Acoustics, USA, Elsevier Academic Press, 2006. 181 • MEHTA & JOHNSON & ROCAFORT, Madan & James & Jorge, Architectural Acoustics - Principles and Design, USA, Prentice-Hall Inc., 1999. • MÜLLER, Helmut A., Die wissenschaftlichen Grundlagen der Raumakustik, Stuttgart, Hirzel Verlag, 1978. • PASCHA, Khaled Saleh, Gefrorene Musik, Berlin, Dissertation for a Doctor in Engeneering, 2004. • ROSSI, Mario, Audio, Lausanne, Presses polytechnique et universitaires romandes, 2007. • THOMPSON, Emily, The Soundscape of Modernity, USA, The MIT Press, 2002. • XENAKIS, Iannis, musique de l’architecture, Marseilles, Editions Parenthèses, 2006. • ZIMMERMANN & ZUMSTEIN, Marc & Simon, Une salle de concert et un hôtel à Burgdorf, Lausanne, Projet de Master EPFL, 1998. 182 183 index INDEX A Absorption Acoustical area Amsterdam Concertgebouw 55 57, 86 112 Ando, Yoichi xii Aspendum Theater at Aspendum 91 Asymmetric. See Form Athens Odeon of Agrippa 90 Berlin Berlin Philharmonie 148 Kammermusiksaal 168 Konzerthaus Berlin 102 Musikhochschule Konzertsaal134 Birmingham Symphony Hall 174 Bloomington Indiana University Auditorium 177 Bonn Beethovenhalle 144 Boston Symphony Hall 117 B BR. See Bass ratio Baltimore Joseph Meyerhoff Symphony Hall Bristol Colston Hall 130 Brussels Palais des Beaux-Arts 122 Budapest Pátria Hall 163 Buenos Aires Teatro Colón 118 Buffalo Kleinhans Music Hall 128 159 Baroque music 16 Baroque period 15 Basel Stadtcasino Bass ratio 100 87 Bayreuth Festspielhaus 108 Beranek, Leo 22 187 C D California Segerstrom Hall Dallas Eugene McDermott Concert Hall 166 169 Caracas Aula Magna 135 Cathedral 11 Chicago Orchestra Hall E 114 Christenchurch Christenchurch Town Hall 150 Church Circumfluent. arrangement 9, 10, 13, 15 See Seating Classical music 17 Classical period 17 Cleveland Severance Hall 124 Concert Concert hall Constantinople Church of St. Sophia Copenhagen Radiohuset, Studio 1 Tivoli Koncertsal 188 Index Diamond. See Form Early Christian period Early-decay-time Edinburgh Usher Hall 9 86 119 Edmonton Northern Alberta Jubilee Auditorium 143 EDT. See Early-decay-time Elliptic. See Form 34 17, 21 93 Ensemble 70 Envelopment 62 Epidaurus Theater at Epidaurus F Field of interest 129 140 88, 89 Form Asymmetric Diamond Elliptic xii 37 37, 81 37 Fan Freeform Horseshoe Semi circle Semi elliptic Shoebox 36 37 17, 36 36 36 19, 36 IACC. See interaural correlation coefficient cross- Initial-time-delay gap 60, 87 Instrumental music Freeform. See Form Frequency I 55 Frontal. See Seating arrangement 16 Interaural cross-correlation coefficient 86 Intimacy 60, 87 G Geneva Victoria Hall Glasgow St. Andrew Hall Gothenburg Konserthus J 115 109 125 Gothic period 11 Greek period 7 H Helsinki Kulttuuritalo Hertz Horseshoe. See Form 141 55 Jerusalem Binyanei Ha’Oomah 146 L La Chaux-de-Fonds Salle Musica 136 Lateral. See Seating arrangement Leipzig Gewandhaus neues Gewandhaus 157 110 Liverpool Philharmonic Hall 127 London Barbican Hall Royal Albert Hall Royal Concert Hall Royal Festival Hall 158 106 173 132 189 Royal Opera House Loudness 104 86 M New York Avery Fisher Hall Carnegie Hall Eastman Theatre Metropolitan Opera House Manchester Free Trade Hall 131 Massachusetts Seiji Ozawa Hall Tanglewood Music Shed 176 126 Opera Methodology xiii Osaka Symphony Hall Mexico City Sala Nezahualcoyotl 155 17 101 Minneapolis Minnesota Orchestra Hall 153 Monody Munich Herkulessaal Philharmonie am Gasteig Mystery play Index 45 11 9 133 164 11 147 113 120 111 O Odea Milan Alla Scala La Scalla Teatro alla Scala Miracle play 190 N Organum 7 15, 17 10 162 P Paris Cathédrale Notre-Dame Opéra Bastille Opéra Garnier Salle Pléyel Parma Teatro Farnese Philadelphia Academy of Music 95 171 107 121 98 137 Plainchant 11 Polyphony 11 Problematics xi Program 79 Reflection 55 Circumfluent Frontal Lateral Renaissance 13 Semi circle. See Form R Reverberation time 22, 56, 85 Romanesque Period 10 Roman period 40 40 40 Semi elliptic. See Form Shoebox. See Form 7 Site 77 Romantic music 19 Song 31 Romantic period 19 Sound 53 Rome Church of St. Peter sound wave 54 92 Spaciousness 86 Speech 16 Strength factor 86 Rotterdam De Doelen Concertgebouw 149 Stuttgart Neue Liederhalle S Sabbioneta Teatro Sabbioneta 139 97 Surface diffusicity index 62 Sabine, Wallace Clement 5, 22 Surface diffusivity index 86 Salt Lake City Abravanel Symphony Hall 156 Sydney Sydney Opera House Salzburg Festspielhaus 145 T San Francisco War Memorial Opera House 123 Schelling, Friedrich 151 4 Taipei Cultural Centre Concert Hall167 Tel Aviv Frederic R. Mann Auditorium142 SDI. See Surface diffusivity index Theater Seating arrangement Tokyo 7, 13, 15, 21, 34 191 Bunka Kaikan Hamarikyu Asahi Hall Metropolitan Art Space NHK Hall Orchard Hall Suntory 154 175 172 152 170 165 Toronto Roy Thompson Hall 160 V Venice Basilica di San Marco Alla Scala Teatro di Giovanni e Paolo 94 17 99 Vicenza Teatro Olympico 96 Vienna Grosser Musikvereinssaal Staatsoper Vineyard-style Vitruvius, Pollio 105 138 71, 81 8 W Wales St. David’s Hall Warmth Worcester Mechanics Hall 192 Index 161 61, 87 103 Z Zurich Grosser Tonhallesaal 116 193 Since this book is a work that was created as a frozen image of a research that is still in progress, there is no final conclusion. But I would like to thank a number of people that helped me during this work with important comments and aid for the creation of this book: Jeffrey Huang for having me accepted as a master student. Hervé Lissek for important help on acoustical questions. Nathaniel Zuelzke for countless comments and correction of this current paper and the actual advancement of the research. my brother for drawing some of these schemes. my father and my mother for giving me general hints for comprehension problems. and ... numerous friends for helpful comments, hints and discussions on representation, formulation and the problematics of acoustics and concert hall design.