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Acoustics 08 Experimental analysis of the acoustical behaviour of Musikverein in concert and ballet configurations A. Farina, D. E. Commins and N. Prodi (a) University of Parma, Via delle Scienze 181/A, Industrial Engineering Dept., 43100


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Acoustics 08

Experimental analysis

  • f the acoustical behaviour of Musikverein in

concert and ballet configurations

  • A. Farina, D. E. Commins and N. Prodi

(a) University of Parma, Via delle Scienze 181/A, Industrial Engineering Dept., 43100 Parma, Italy (b) Commins Acoustics Workshop, 15 rue Laurence Savart, 75020 Paris, France (c) Engineering Dept. - Univ. of Ferrara, Via Saragat, 1, 44100 Ferrara, Italy

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Topics

Configurations of the room Standard room acoustics measurements Coupling with the storage space under the stalls Surface intensity measurements Analysis of the results

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Concert configuration

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Concert configuration

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Ballroom configuration

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Ballroom configuration

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Measurement method: Exponential Sine Sweep

Portable PC with 4 - channels sound board Original Room SoundField Microphone B- format 4 - channels signal (WXYZ) Measurement of B - format Impulse Responses MLS excitation signal Portable PC with additional sound card Room Microphone Output signal y Measurement of room Impulse Response Sweep test signal x Loudspeaker

Not-linear, time variant system K[x(t)] Noise n(t) input x(t)

+

  • utput y(t)

linear system w(t)⊗h(t) distorted signal w(t)

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SLIDE 8

Exponential Sine Sweep method

x(t) is a sine signal, which frequency is varied exponentially with time, starting at f1 and ending at f2.

⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ ⎛ − ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⋅ ⋅ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⋅ ⋅ ⋅ 1 ln ln 2 sin

1 2 1 2 1

f f T t e f f T f π = x(t)

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Test Signal – x(t)

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Measured signal - y(t)

The not-linear behaviour of the loudspeaker causes

many harmonics to appear

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Inverse Filter – z(t)

The deconvolution of the IR is obtained convolving the measured signal y(t) with the inverse filter z(t) [equalized, time-reversed x(t)]

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Deconvolution of Exponential Sine Sweep

The “time reversal mirror” technique is employed: the system’s impulse response is obtained by convolving the measured signal y(t) with the time-reversal of the test signal x(-t). As the exp. sine sweep does not have a “white” spectrum, proper equalization is required Test Signal x(t) Inverse Filter z(t)

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Result of the deconvolution

The last impulse response is the linear one, the preceding are the harmonics distortion products of various orders 1° 2° 3° 5°

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IR Selection

After the sequence of impulse responses has been

  • btained, it is possible to select and insulate just one of

them:

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Maximum Length Sequence vs. Sweep

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Hardware: loudspeaker & microphone

Dodechaedron loudspeaker Soundfield microphone

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Equipment: computer & sound interface

Laptop PC MOTU Traveler

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Directivity of transducers

  • 40
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5

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30 60 90 120 150 180 210 240 270 300 330

1000 Hz

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5

  • 1
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30 60 90 120 150 180 210 240 270 300 330

2000 Hz

LookLine D200 dodechaedron

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5

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30 60 90 120 150 180 210 240 270 300 330

250 Hz

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5

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30 60 90 120 150 180 210 240 270 300 330

4000 Hz

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5

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30 60 90 120 150 180 210 240 270 300 330

8000 Hz

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5

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30 60 90 120 150 180 210 240 270 300 330

16000 Hz

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SLIDE 19

pressure-velocity microphone

  • The Soundfield microphone allows for simultaneous measurements
  • f the omnidirectional pressure and of the three cartesian components
  • f particle velocity (figure-of-8 patterns)
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Directivity of transducers

Soundfield ST-250 microphone

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

125 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

250 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

500 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

1000 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

2000 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

4000 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

8000 Hz

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6

30 60 90 120 150 180 210 240 270 300 330

16000 Hz

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Measurement method: B-format Impulse Response

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3D Impulse Response (Gerzon, 1975)

Portable PC with 4- channels sound board Original Room Sound Source SoundField Microphone B-format 4-channels signal (WXYZ) Measurement of B-format Impulse Responses MLS or sweep excitation signal Convolution of dry signals with the B-format Impulse Responses Sound Source Mono Mic. B-format Imp. Resp.

  • f the original room

B-format 4-channels signal (WXYZ) Convolver Ambisonics decoder Speaker array in the reproduction room

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Measurement positions

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ISO3382 Parameters

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Results

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Results

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Results

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Results

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Results

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Storage room under the stalls

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Sound reduction index Sound reduction index

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Reverberation time of storage room (empty)

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Surface Sound Intensity

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Surface Sound Intensity

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Conclusions

Musikverein is a truly variable acoustics room The Ballroom configuration exhibit reverberation times significantly

larger than the Concert configuration, particularly at medium frequencies

Also G is significantly different However, C80 and LF do not change remarkably, ensuring good

acoustical quality also in Ballroom configuration

The storage room under the stalls is heavily insulated, hence it cannot

have any effect

The effect of the audience should be taken into account, particularly in

Ballroom configuration, where it would be probably much larger than in Concert configuration.