Concert halls conveyors of musical expressions

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Communication Acoustics: Paper ICA216-465 Concert halls conveyors of musical expressions Tapio Lokki (a) (a) Aalto University, Dept. of Computer Science, Finland, tapio.lokki@aalto.fi Abstract: The first question of an acoustician regarding a new concert hall is too often: What is the reverberation time? Such tradition has historical reasons as reverberation time and sound strength have been considered the most important objective measures of concert halls. However, although they are indeed important music should be loud enough and reverberated to sound good they do not tell much on the multidimensional acoustical conditions of a hall. This paper collects the recent research to understand concert hall acoustics beyond these traditional measures. The results indicate that a concert hall is considered exceptional if it renders music expressive, i.e., conveys the subtle nuances of music from the stage to the audience as well as possible. In other words, a concert hall is preferred if it renders proximate sound with large dynamics and wide frequency range. This paper links together musical acoustics, room acoustics and human spatial hearing to highlight recent findings in concert hall acoustics research. Keywords: auditorium acoustics, music, concert halls, dynamics

Concert halls conveyors of musical expressions 1 Introduction The audience gathers to concert halls to listen to music in favorable acoustic conditions. The hall conveys the sound waves from the stage to the audience areas. The reverberation of the hall ties consecutive notes together and provides continuity to the music. In addition, the reflections from room boundaries make the sound stronger. Moreover, the concert hall isolates the music from distracting noise leaving room for full dynamics that an orchestra provides. In short, a concert hall can be considered as a conveyor of music from the orchestra to the audience. In communication acoustics, such a process is often described with a source-medium-receiver model [1], illustrated in Fig. 1 in the case of a concert hall. Research on concert hall acoustics is often focused on the medium part of this communication chain. Objective room acoustics research is performed with measured or modeled impulse responses. Such an impulse response completely describes this linear and time-invariant communication channel from one source to one receiving position. Typically, the linear and timeinvariant assumption is indeed valid, as the temperature is not changing and there are no currents in the air. The ISO3382-1:29 standard [2] defines that the impulse response should be measured with good quality transducers that have flat frequency response to all directions, i.e., an omnidirectional point source (usually a special loudspeaker) and an omnidirectional measurement microphone. However, in an orchestra there are no omnidirectional sources as all musical instruments have frequency dependent radiation patterns [3, 4]. In addition, receivers human listeners have two ears and human spatial hearing has frequency dependent characteristics [5]. In the standard [2], there are a few parameters that are computed from impulse responses captured with directional devices, such as a figure-of-eight microphone or a dummy head, to better mimic the spatial aspects of human hearing. However, the standard falls short of linking the subjective impressions and objective measurements completely [6, 7, 8]. Figure 1: Source - Medium - Receiver communication chain in the case of a concert hall. 2

One aspect which is totally ignored in the ISO3382 standard, and indeed often in concert hall acoustics research, is that both the source and the receiver have level dependent effects. Therefore, the studies restricted to room impulse responses are inadequate, as both the source signals and human hearing have non-linear characteristics. As indicated in Fig. 1 the spectrum of the source signal is level dependent, meaning that the spectrum of the orchestra is different in different playing dynamics, even if the same instruments would play the same notes [9]. In addition, human hearing has level dependent sensitivity, which is generally known in the form of Equal Loudness Contours [1], but again this phenomenon is not taken into account in concert hall acoustics research. Thus, the communication chain has a non-linear source, a linear medium, and a non-linear receiver, making the interpretation of the measured impulse responses very hard. More importantly, these non-linearities affect strongly how a concert hall renders the music. This paper addresses one of these level dependent issues. 2 Music expressions of composers A concert hall is a dedicated space for a music performance, which is carried out with acoustic, non-amplified instruments. The music itself expresses the ideas and feelings of a composer who has chosen the instruments and notes they played. Generally speaking, the music consists of tempo, harmony, rhythm, timbre, and accents to name a few. In symphony, these features form the music and can wake up emotions in the listener, when the composer has been successful and the performing artists master their instruments and ensemble playing. As said above, the role of a concert hall is to render music so that the message by a composer is delivered as well as possible to the audience. The message often includes emotional passages and in the best case the hall supports the played music making it warm, bright, dynamic, and intimate. In traditional research on concert halls these aspects are mainly ignored. The research is concentrated on analysis of room impulse responses and such parameters as strength, reverberation, clarity, auditory source width, and envelopment have been considered important [2]. All these measures are computed from the decay of room reverberation and they do not tell much on timbral (warmth and brightness) or level dependent (dynamics) aspects. However, some papers have noticed, e.g., the importance of lateral reflections to spatial impression [11, 12, 13, 14], but clear connection between music and room acoustics has been missing. Two years ago the first article [9] linked the whole communication chain (Fig.1) together, by explaining why some concert halls produce larger perceived dynamics than the others. In that article, it was shown that in fortissimo playing the instruments emits much more harmonics, i.e., high frequencies than in pianissimo. Moreover, the form of a human head strengthens these high frequencies for the sound coming from the side, thus showing the benefit of lateral reflections instead of reflections from the ceiling. 3

3 Level dependent spectra of a source and a receiver The importance of high frequencies for large dynamics has been recently discussed [9, 15, 16], but the origins of warm and strong bass sound has not received much attention. As well known, the warm sound is related to the strength and quality of low frequencies, but the measurements are usually done only at 125 Hz octave band [17], which is clearly not sufficient. There are many instruments that emit a lot of sound below 9 Hz and this frequency region is extremely important for warm and emotional sound. Figure 2 illustrates the spectral differences of piano and fortissimo of a full orchestra. The data are analyzed from 29 recordings of Bruckner s 4th Symphony (bars 19-26, III movement). This passage is good for such analysis as the orchestra plays a long crescendo practically without changing the played notes, see more details in [9]. In Fig. 2 the spectra at different dynamics are aligned so that they overlap at 1 khz. It can be clearly seen that in fortissimo there are relatively more low frequencies. What is relevant here is that when the overall level increase is removed, we can see that in fortissimo both low and high frequencies are pronounced. In other words, the change in level is not the same at different frequencies, i.e., the spectrum changes its shape. Thus, as indicated in Fig. 1 the spectrum of the excitation signal in a concert hall is level dependent. Another level dependent phenomenon is related to human hearing, i.e., the receiver in a concert hall. The sensitivity of human hearing at different levels is illustrated on the right in Fig. 2. Again, the spectra of equal loudness contours are aligned to match at 1 khz, and such illustration shows that the higher the level is the flatter the equal loudness contour is. Relative magnitude [db] 1-1 -2-3 -4-5 Spectra of full orchestra sound Fortissimo Piano "Relative loudness" [sones] 5 4 3 2 1-1 Equal Loudness Contours 4 db 65 db 75 db 85 db 95 db Figure 2: Left: The spectra of a full orchestra sound in different dynamics. Right: Relative magnitude responses of equal loudness contours. Note that in both figures the curves are shifted to overlap at 1 khz. When these two level dependent effects are combined together, the result is quite interesting as shown in Fig. 3. In this figure, the spectrum of piano level has been added to the equal loudness contour of 4 db and the spectrum of fortissimo level has been added to several higher level equal loudness contours, and finally the plot shows differences between these curves. The figure illustrates that when an orchestra plays in fortissimo the low frequencies below 2 Hz and high frequencies above 3 khz are substantially pronounced in comparison 4

Relative magnitude [db] 3 25 2 15 1 5 Change in frequency response (re. 4dB equal loudness contour) w/o Eq. Loud. Curves +25 db +35 db +45 db +55 db -5 Figure 3: Illustration of how the relative magnitudes of different frequencies change when an orchestra plays the same notes in fortissimo and in piano. The black curve is the difference without the effects equal loudness contours. If the spectra in piano and in fortissimo would be the same then the result in this illustration would be a flat line at db. with piano passages. Nevertheless what is the effect of a concert hall, as a linear transfer path of sound when these level dependencies are always present? If a hall attenuates strongly either the low or the high frequencies, then the perceived frequency response is different and in such a case human perception follows different curves of Fig. 3 at different frequency regions. In fact, there are two distinct features and the other one is related to the directivities of sources [18] and receivers [5]. The directivities affect mainly high frequencies and the perceptual consequences have been explained in another article [9]. At low frequencies both sources and receivers are more or less omnidirectional, and only the level dependent features matter. 4 Perceived bass in concert halls Figure 4 shows measured frequency responses from 1 European concert halls. The plotted responses are averages of 25 source positions, thus they represent an orchestra well as a source. The plots reveal that there are level differences of as high as 1 db at low frequencies below 2 Hz. In the light of these differences, Fig. 3 could be interpreted so that a hall that emphasizes 1 db more the low frequencies, the perceived increase is not 1 db, but 5

Frequency responses at 11 meters, average of 25 sources Magnitude [db] 1 5-5 WS BB BK MH VM CP AC BP SB MG -1 Frequency responses at 19 meters, average of 25 sources Magnitude [db] 1 5-5 WS BB BK MH VM CP AC BP SB MG -1 Figure 4: Frequency responses of 1 different concert halls, measured with the loudspeaker orchestra in two different receiver positions. it is about 13 db. This 3 db increase in perceived bass is the consequence of flatter equal loudness contours at higher levels. Our experience is that in halls with weak low frequencies the bass lacks strength while in halls with strong low frequencies the bass instruments sound powerful and intense. Moreover, in large crescendo and fortissimo passages the compositions often includes bass drum, timpani, tuba, and double basses, which all produce warm sound when they are clearly audible. The reasons why some concert halls render much more powerful low frequencies are outside the scope of this article, but they are discussed in the accompanying paper [19]. 5 Conclusions This article contributes to concert hall acoustics research by addressing the level dependent features of the sources and the receivers. These aspects are well known in psychoacoustics, but research on concert halls usually ignores these fundamental issues. In addition, it is shown that when an orchestra plays in different dynamics, not only the overall level changes, but the 6

shape of the frequency spectrum changes. Low and high frequencies are pronounced much more than mid frequencies, resulting in the enhancement of brightness, brilliance, and warmth of the music. It is also evident that these timbral aspects have a key role in making music more intimate and expressive. Acknowledgements This research has received funding from the Academy of Finland, project no. [25799]. In addition, I like to thank the whole Virtual Acoustics research team at Aalto University for their hard work. References [1] V. Pulkki and M. Karjalainen. Communication Acoustics An introduction to speech, audio and psychoacoustics. Wiley, 215. [2] ISO 3382-1. Acoustics measurement of room acoustic parameters part 1: Performance spaces. International Standards Organization, 29. [3] J. Meyer. Acoustics and the Performance of Music. Verlag das Musikinstrument, Frankfurt/- Main, 1978. [4] J. Pätynen, V. Pulkki, and T. Lokki. Anechoic recording system for symphony orchestra. Acta Acustica united with Acustica, 94(6):856 865, 28. [5] J. Blauert. Spatial Hearing. The psychophysics of human sound localization. MIT Press, Cambridge, MA, 2nd edition, 1997. [6] J.S. Bradley. Review of objective room acoustics measures and future needs. Applied Acoustics, 72:713 72, 211. [7] L. Kirkegaard and T. Gulsrud. In search of a new paradigm: How do our parameters and measurement techniques constrain approaches to concert hall design? Acoustics Today, 7(1):7 14, 211. [8] T. Lokki, J. Pätynen, A. Kuusinen, and S. Tervo. Disentangling preference ratings of concert hall acoustics using subjective sensory profiles. Journal of the Acoustical Society of America, 132(5), 212. 3148-3161. [9] J. Pätynen, S. Tervo, P. W. Robinson, and T. Lokki. Concert halls with strong lateral reflections enhance musical dynamics. Proceedings of the National Academy of Sciences of the United States of America (PNAS), 111(12):449 4414, 214. [1] D.W. Robinson and R.S. Dadson. A re-determination of the equal-loudness relations for pure tones. British Journal of Applied Physics, 7:166 181, 1956. [11] A. H. Marshall. A note on the importance of room cross-section in concert halls. Journal of Sound and Vibration, 5(1):1 112, 1967. 7

[12] A. H. Marshall. Levels of reflection masking in concert halls. Journal of Sound and Vibration, 7(1):116 118, 1968. [13] M. Barron. The subjective effects of first reflections in concert halls the need for lateral reflections. Journal of Sound and Vibration, 15(4):475 494, 1971. [14] M. Barron and A.H. Marshall. Spatial impression due to early lateral reflections in concert halls: The derivation of a phisical measure. 77(2):211 232, 1981. [15] T. Lokki and J. Pätynen. The acoustics of a concert hall as a linear problem. Europhysics News, 46(1):13 17, 215. [16] T. Lokki, J. Pätynen, S. Tervo, A. Kuusinen, H. Tahvanainen, and A. Haapaniemi. The secret of the musikverein and other shoebox concert halls. In The 9th International Conference on Auditorium Acoustics, Paris, France, October 29-31 215. [17] L. Beranek. Concert Halls and Opera Houses: Music, Acoustics, and Architecture. Springer- Verlag (New York), 2nd edition, 24. 664 pages. [18] J. Pätynen and T. Lokki. Directivities of symphony orchestra instruments. Acta Acustica united with Acustica, 96(1):138 167, 21. [19] T. Lokki. Why some concert halls render music more expressive and impressive than the others? In International Symposium on Musical and Room Acoustics (ISMRA), La Plata, Argentina, September 11-13 216. 8