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A DIAGNOSTIC SYSTEM MEASURING ORTHOGONAL FACTORS OF SOUND FIELDS IN A SCALE MODEL OF AUDITORIUM
Journal of Sound and < ibration (2000) 232(1), 231}237
doi:10.1006/jsvi.1999.2695, available online at http://www.idealibrary.com on
A DIAGNOSTIC SYSTEM MEASURING ORTHOGONAL
FACTORS OF SOUND FIELDS IN A SCALE MODEL
OF AUDITORIUM
M. S AKURAI
Graduate School of Science and ¹ echnology , Kobe ; niversity , I Rokkodai , Nada ,
Kobe 657-8501, Japan and > oshimasa Electronic Inc ., 1-58-10 > oyogi ,
Shibuya , ¹ okyo 151-0053, Japan
S. A IZAWA
> oshimasa Electronic Inc ., 1-58-10 > oyogi , Shibuya , ¹ okyo 151-0053, Japan
AND
Y. S UZUMURA AND Y. A NDO
Graduate School of Science and ¹ echnology , Kobe ; niversity , I Rokkodai , Nada ,
Kobe 657-8501, Japan
( Accepted 30 June 1999)
Based on the model of auditory}brain system which consists of the
autocorrelation mechanism, the interaural cross-correlation mechanism between
both the auditory pathways, and the specialization of human cerebral hemispheres
(Y. Ando 1998 Architectural Acoustics , Blending Sound Sources , Sound Fields , and
¸ isteners New York: AIP Press/Springer-Verlag), a new diagnostic system was
developed. After obtaining the binaural impulse response, four orthogonal factors
including the SP ¸, the initial time-delay gap between the direct sound and the "rst
re#ection, the subsequent reverberation time and the IACC can be analyzed for the
calculation of the scale values of both global and individual subjective preferences.
In addition, two more factors extracted from the interaural cross-correlation
function
and =
IACC
, can be "gured out. Also, the sound energy,
U
(0), the
, and "ne structures of autocorrelation function of sound
signals including the magnitude of "rst maximum,
q e
, can be
analyzed. As an example of the measurement, e!ects of re#ectors' array above the
stage in a 1/10 scale model of auditorium at each seat are discussed here.
(
/ 1
, and its delay time,
q 1
2000 Academic Press
IACC
[1}6] , and also the running ACF of sound "eld at each seat in a scale model as well
as in a real auditorium, a diagnostic system is developed. Based on the model of
D ¹
, ¹
sub
, IACC ,
q IACC
, and =
0022-460X/00/160231#07 $35.00/0
(
2000 Academic Press
q IACC
e!ective duration,
1. INTRODUCTION
In order to measure orthogonal factors, SP ¸,
1
8112153.005.png 8112153.006.png 8112153.007.png 8112153.008.png
232
M. SAKURAI E ¹ A ¸.
Figure 1. A model of auditory}brain system.
auditory}brain system which consists of the autocorrelation mechanism, the
interaural cross-correlation mechanism between both the auditory pathways, and
the specialization of human cerebral hemispheres as shown in Figure 1 [1],
a diagnostic system was designed. The system works on PC for Windows with
AD&DA converters; there is no need for special additional devices. After obtaining
the binaural impulse responses, four orthogonal factors including the SP ¸, the
initial time-delay gap between the direct sound and the "rst re#ection, the
subsequent reverberation time and the IACC are analyzed. These factors are used
for the calculation of the scale values of both the global and individual subjective
preferences. In addition to the four factors, two more factors,
q IACC
and =
U
(0), the e!ective duration,
,de"ned by the delay at which the envelope of normalized ACF becomes 0)1 (see
Figure 3), and "ne structures of autocorrelation function of sound signals including
the magnitude of "rst maximum,
, of source signals are
analyzed. In order to examine e!ects of the re#ectors' array above the stage in a
, and its delay time,
q 1
10
scale model of auditorium, the IACC measurements are demonstrated here.
2. OUTLINE OF A DIAGNOSTIC SYSTEM
Because the complex requirements made the system di$cult to evaluate, an
advanced diagnostic system and a high-power computer was used. The measuring
system was utilized to obtain the binaural impulse response at each listening
as
de"ned in Figure 2, extracted from the interaural cross-correlation function can be
"gured out for evaluating the image shift of sound source and the apparent source
width [6] respectively. Also, the averaged sound energy,
IACC
q e
/ 1
8112153.001.png
A DIAGNOSTIC SYSTEM FOR SOUND FIELDS
233
Figure 2. De"nitions of the IACC ,
q IACC
and =
IACC
in the interaural cross-correlation function.
Figure 3. A practical example of determining e!ective duration of ACF de"ned by the ten-
percentile delay, with the straight line-"tting envelope of ACF from 0 to !5 dB.
10
scale model of dummy head (a sphere with a diameter of 25 mm) was sampled after
passing through a low-pass "lter (see Figure 4) . The binaural-impulse-response
measurement may be performed by a summation of the output data from the linear
system, without any multiplication operation [7, 8]. The measurement was done
automatically within only a few seconds by pushing a single button. It took another
few seconds for the analysis of the orthogonal acoustic factors and the scale value of
the subjective preference. And at the same time this program can take the result to
compute the acoustic parameters and prepare the reports.
position. The sound was created by using an omni-directional loudspeaker fed with
a maximum length signal produced by a diagnostic system in a notebook PC. The
period of the maximum length signal (MLS) was between 1024 and 524 288
samples, and the sampling rate can be changed between 8 and 48 kHz. The acoustic
signal ampli"ed from the two microphones placed at the entrances of ears of a
8112153.002.png
234
M. SAKURAI E ¹ A ¸.
Figure 4. A block diagram of the measurement system.
Figure 5. An example of display window of the diagnostic system, with binaural impulse responses.
8112153.003.png
A DIAGNOSTIC SYSTEM FOR SOUND FIELDS
235
3. MEASUREMENT OF ORTHOGONAL ACOUSTIC FACTORS
3.1. PROCEDURE
The diagnostic system developed may examine e!ects of scattered re#ections of
complex boundary conditions of the room. The re#ectors above the stage are
designed mainly for the performer obtaining the preferred re#ections according to
the program sources. We measured the IACC of the sound "eld at each seat to "nd
the e!ects of the re#ectors' array above the stage [9] . The e!ective direction of
re#ections to listeners for the 2000 Hz range is centered on $183 from the median
plane, which might be realized by a re#ectors above the stage [1] . Therefore, the
IACC of the 2000 Hz frequency band is selected here to be examined.
In order to obtain reliable results, measurements were repeated several times
until the same results for the binaural impulse responses were obtained. The sound
is produced by using an omni-directional loudspeaker fed with the MLS produced
by the diagnostic system in a notebook PC. Figure 5 shows the window on PC of
actual diagnostic system with the data obtained from the impulse responses. In the
measurement, special attention should be paid to maintain a suitable value of the
signal-to-noise ratio adjusting the power level of the loudspeaker.
Figure 6. Measured IACC for the 2000 Hz frequency band with re#ectors above the stage.
 
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