Dynamic Spatial Responsiveness in Concert Halls

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Dynamic Spatial Responsiveness in Concert Halls acoustics Article Dynamic Spatial Responsiveness in Concert Halls Evan Green * and Eckhard Kahle Kahle Acoustics, 1050 Brussels, Belgium * Correspondence: [email protected]; Tel.: +32-2-345-10-10 Received: 30 May 2019; Accepted: 2 July 2019; Published: 22 July 2019 Abstract: In musical perception, a proportion of the reflected sound energy arriving at the ear is not consciously perceived. Investigations by Wettschurek in the 1970s showed the detectability to be dependent on the overall loudness and direction of arrival of reflected sound. The relationship Wettschurek found between reflection detectability, listening level, and direction of arrival correlates well with the subjective progression of spatial response during a musical crescendo: from frontal at pianissimo, through increasing apparent source width, to a fully present room acoustic at forte. “Dynamic spatial responsiveness” was mentioned in some of the earliest psychoacoustics research and recent work indicates that it is a key factor in acoustical preference. This article describes measurements of perception thresholds made using a binaural virtual acoustics system—these show good agreement with Wettschurek’s results. The perception measurements indicate that the subjective effect of reflections varies with overall listening level, even when the reflection level, delay, and direction relative to the direct sound are maintained. Reflections which are perceptually fused with the source may at louder overall listening levels become allocated to the room presence. An algorithm has been developed to visualize dynamic spatial responsiveness—i.e., which aspects of a three-dimensional (3D) Room Impulse Response would be detectable at different dynamic levels—and has been applied to measured concert hall impulse responses. Keywords: auditorium acoustics; dynamics; spaciousness; spatial response; auditory perception 1. Introduction 1.1. (Dynamic) Spatial Responsiveness Musicians and conductors consider the concert hall part of their instrument—it is a tool for musical expression, with the best concert halls enhancing the range of expression. The deliberate variation of intensity—in other words, changes in musical dynamics—is a key ingredient in most musical composition and performance. Without both strong and subtle dynamic changes, much musical and emotional intensity is lost. Playing a musical instrument with more intensity generates not only an increase in objective sound level, but also changes in the frequency spectrum of the sound. The connection between musical dynamics and spatial impression was observed in some of the earliest research into psychoacoustics. Marshall [1] writes in 1966 that “as a property of the hall, [spatial impression] relates to loudness attributes ::: for the listener, it generates a sense of envelopment in the sound and of direct involvement with it”, with similar observations being made by Keet [2] and Barron [3]. Writing in 1978, Kuhl [4] states that (translated from German) “[spatial impression] is only, if at all, present in forte passages. Musical dynamics therefore not only influence the loudness, but with a sufficient spatial responsiveness, they increase the involvement of the room in the music. For the lay-listener, who is perhaps not even aware of this effect, this spaciousness is an unconscious yet pleasant experience.” In certain conditions therefore, increases in dynamics can generate an additional dimension of spatial impression for the listener—changes in the spatial impression due to changes in dynamics will be referred to here as “dynamic spatial responsiveness”. Acoustics 2019, 1, 549–560; doi:10.3390/acoustics1030031 www.mdpi.com/journal/acoustics AcousticsAcoustics 20192019,, 21 FOR PEER REVIEW 5502 Spatial impression, apparent source width (ASW), and listener envelopment (LEV) have been studiedSpatial in much impression, detail [3,5–10], apparent with source typical width approach (ASW),es using and listener either energy envelopment integrals (LEV) over haverelatively been longstudied time in intervals much detail (for [3example,,5–10], with “early” typical (0–80 approaches ms) or “late” using (0 either ms to energy infinity) integrals time ranges) over relatively and/or largelong timeangular intervals ranges (for (such example, as in “early”the definition (0–80 ms) of Lateral or “late” Fraction), (0 ms to infinity)or considering time ranges) spatial and effects/or large as staticangular and ranges unchanging (such aswith in theperformance definition dynamics. of Lateral Fraction),While valuable or considering results have spatial been e ffachieved,ects as static the formerand unchanging approach “bundles” with performance energy from dynamics. different While times valuable and directions results have and does been not achieved, take into the account former theapproach differing “bundles” sensitivity energy of our from hearing different to reflecti timesons and from directions different and directions, does not take and intonor accountis masking the factoreddiffering in: sensitivity when long of our time hearing ranges to and reflections large angu fromlar di ffrangeserent directions, are integrated, and nor the is (potentially masking factored very important)in: when long details time of ranges what happens and large in angular those rang rangeses remain are integrated, unclear. the The (potentially latter approach very important)overlooks thedetails importance of what happensof dynamics in those and rangesits importance remain unclear.in the subjective The latter acoustical approach quality overlooks of concert the importance halls. of dynamicsRecently, and the its research importance group in theat Aalto subjective Universi acousticalty has qualitytaken up of concertthe topic halls. of dynamics anew, demonstratingRecently, thethat researchdynamic group spatial at responsiveness Aalto University is related has taken to changes up the topicin instrument of dynamics frequency anew, responsesdemonstrating and directivity that dynamic at higher spatial dynamic responsiveness levels [11–14]: is related due to to greater changes binaural in instrument sensitivity frequency to high frequenciesresponses and at lateral directivity angles, at higheran increased dynamic spatial levels impression [11–14]: due results to greater from binauralthe additional sensitivity higher to harmonicshigh frequencies that are at generated lateral angles, when an instruments increased spatial are played impression loudly. results However, from little-known the additional research higher publishedharmonics by that Wettschurek are generated [15] when in instruments1978 demonst arerates played that loudly. the connection However, little-knownbetween dynamics, research loudness,published and by Wettschurek spatial impression [15] in 1978 is linked demonstrates to other thatfundamental the connection processes between in the dynamics, human loudness,hearing system,and spatial in particular impression how is reflections linked to from other differen fundamentalt directions processes are masked in the or human unmasked hearing at different system, overallin particular listening how (dynamic) reflections levels. from different directions are masked or unmasked at different overall listening (dynamic) levels. 1.2. Research by Wettschurek 1.2. Research by Wettschurek In Wettschurek’s thesis [15], he describes an experiment to determine the perception threshold In Wettschurek’s thesis [15], he describes an experiment to determine the perception threshold of of a test reflection dependent on overall listening levels. The experiment is shown diagrammatically a test reflection dependent on overall listening levels. The experiment is shown diagrammatically in in Figure 1. Figure1. FigureFigure 1. 1. DiagrammaticDiagrammatic representation representation of of an an experiment experiment to to determine determine the the perception perception threshold threshold of ofa reflectiona reflection E Ein inthe the presence presence of of direct direct sound sound D, D, a alateral lateral reflection reflection R, R, and and reverberation reverberation H. H. After After WettschurekWettschurek [15]. [15]. AA synthetic soundsound fieldfield was was generated generated in anin anechoican anechoic environment environment consisting consisting of the of direct the sound,direct sound,a 2 s reverberation a 2 second reverberation starting at 50 starting ms, and at two 50 ms, discrete and two reflections: discrete one reflections: reflection one being reflection a fixed being lateral a fixedreflection lateral at reflection 60◦ azimuth at 60° and azimuth 30 ms delay, and 30 and ms the delay, other and a test the reflection other a test at 70 reflection ms and ofat variable70 ms and level of variableand variable level position.and variable The position direct sound,. The direct lateral sound, reflection, lateral and reflection, reverberation and reverberation levels were set levels to achieve were seta direct-to-reverberant to achieve a direct-to-reverberant ratio of 0 dB. Withratio anechoicof 0 dB. With speech anechoic used as speech source used material, as source the overall material, sound the overalllevel at sound the listening level at position the listening (“listening position level”) (“listening was adjusted level”) in was the rangeadjusted 20–80 in the dB inrange 5 dB 20–80 increments, dB in 5subsequently dB increments, the subsequently level of the the test level reflection of the wastest reflection adjusted towas establish adjusted the to perceptionestablish the threshold perception of thresholdthis
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