The analytical passive time reversal method (APTRM) is a powerful technique for sound source localization. In that technique, it generally requires that the frequency response function relating the measurement point to the focusing point should be known in advance. However, inside an enclosure of arbitrary shape, there is no theoretical formulation of this frequency response function, and using the APTRM with the free-field Green's function might lead to inaccurate localization of sound sources. This paper proposes a method combining the APTRM with the equivalent source method (ESM) to locate sound sources in an enclosure of arbitrary shape. In this method, the frequency response function relating the measurement point to the focusing point inside the enclosure is first calculated numerically using the ESM, and then the APTRM with this numerical frequency response function is used to realize the localization of sound sources. Numerical simulations in a rectangular enclosure and an enclosure of arbitrary shape as well as an experiment in a rectangular wooden cabinet are performed to verify the validity of the proposed method. The results demonstrate that the frequency response function in an enclosure can be accurately calculated using the ESM; based on measurements with a spherical array composed of 48 microphones, the proposed method can effectively locate the sound sources in enclosures of different shapes and work stably under the situation of low signal-to-noise ratio.

References

1.
Fahy
,
F. J.
,
1977
, “
Measurement of Acoustic Intensity Using the Cross-Spectral Density of Two Microphone Signals
,”
J. Acoust. Soc. Am.
,
62
(
4
), pp.
1057
1059
.
2.
Williams
,
E. G.
,
Maynard
,
J. D.
, and
Skudrzyk
,
E.
,
1980
, “
Sound Source Reconstructions Using a Microphone Array
,”
J. Acoust. Soc. Am.
,
68
(
1
), pp.
340
344
.
3.
Loyau
,
T.
,
Pascal
,
J.
, and
Gaillard
,
P.
,
1988
, “
Broadband Acoustic Holography Reconstruction From Acoustic Intensity Measurements—I: Principle of the Method
,”
J. Acoust. Soc. Am.
,
84
(
5
), pp.
1744
1750
.
4.
Wang
,
Z.
, and
Wu
,
S. F.
,
1997
, “
Helmholtz Equation-Least Method for Reconstructing the Acoustic Pressure Field
,”
J. Acoust. Soc. Am.
,
102
(
4
), pp.
2020
2032
.
5.
Bi
,
C. X.
,
Chen
,
X. Z.
,
Chen
,
J.
, and
Zhou
,
R.
,
2005
, “
Nearfield Acoustic Holography Based on the Equivalent Source Method
,”
Sci. China, Ser. E: Eng. Mater. Sci.
,
48
(
3
), pp.
338
353
.
6.
Duraiswami
,
R.
,
Zotkin
,
D.
,
Borovikov
,
E. A.
, and
Davis
,
L. S.
,
2000
, “
Active Source Location and Beamforming
,”
J. Acoust. Soc. Am.
,
107
(
5
), p.
2790
.
7.
Chen
,
J. C.
,
Yao
,
K.
, and
Hudson
,
R. E.
,
2003
, “
Acoustic Source Localization and Beamforming: Theory and Practice
,”
EURASIP J. Adv. Signal Process.
,
2003
(
4
), pp.
359
370
.
8.
Williams
,
E. G.
,
1997
, “
The Nearfield Acoustical Holography (NAH) Experimental Method Applied to Vibration and Radiation in Light and Heavy Fluids
,”
Comput. Struct.
,
65
(
3
), pp.
323
335
.
9.
Hu
,
D. Y.
,
Bi
,
C. X.
,
Zhang
,
Y. B.
, and
Geng
,
L.
,
2014
, “
Extension of Planar Nearfield Acoustic Holography for Sound Source Identification in a Noisy Environment
,”
J. Sound Vib.
,
333
(
24
), pp.
6395
6404
.
10.
Fernandez-Grande
,
E.
, and
Jacobsen
,
F.
,
2010
, “
Separation of Radiated Sound Field Components From Waves Scattered by a Source Under Non-Anechoic Conditions
,”
Inter-Noise
, Lisbon, Portugal, June 13–16, pp. 3895–3904.
11.
Hald
,
J.
,
2006
, “
Patch Holography in Cabin Environments Using a Two-Layer Handheld Array With an Extended SONAH Algorithm
,”
Euronoise
, Tampere, Finland, May 30–June 1, pp.
1
8
.
12.
Hald
,
J.
,
2009
, “
Basic Theory and Properties of Statistically Optimized Near-Field Acoustical Holography
,”
J. Acoust. Soc. Am.
,
125
(
4
), pp.
2105
2120
.
13.
Langrenne
,
C.
,
Melon
,
M.
, and
Garcia
,
A.
,
2007
, “
Boundary Element Method for the Acoustic Characterization of a Machine in Bounded Noisy Environment
,”
J. Acoust. Soc. Am.
,
121
(
5
), pp.
2750
2757
.
14.
Langrenne
,
C.
,
Melon
,
M.
, and
Garcia
,
A.
,
2009
, “
Measurement of Confined Acoustic Sources Using Near-Field Acoustic Holography
,”
J. Acoust. Soc. Am.
,
126
(
3
), pp.
1250
1256
.
15.
Langrenne
,
C.
, and
Garcia
,
A.
,
2011
, “
Data Completion Method for Characterization of Sound Sources
,”
J. Acoust. Soc. Am.
,
130
(
4
), pp.
2016
2023
.
16.
Bi
,
C. X.
,
Chen
,
X. Z.
, and
Chen
,
J.
,
2008
, “
Sound Field Separation Technique Based on Equivalent Source Method and Its Application in Nearfield Acoustic Holography
,”
J. Acoust. Soc. Am.
,
123
(
3
), pp.
1472
1478
.
17.
Bi
,
C. X.
,
Hu
,
D. Y.
,
Zhang
,
Y. B.
, and
Jing
,
W. Q.
,
2015
, “
Identification of Active Sources Inside Cavities Using the Equivalent Source Method-Based Free-Field Recovery Technique
,”
J. Sound Vib.
,
346
(
1
), pp.
153
164
.
18.
Bi
,
C. X.
,
Hu
,
D. Y.
,
Zhang
,
Y. B.
, and
Bolton
,
J. S.
,
2013
, “
Reconstruction of the Free-Field Radiation From a Vibrating Structure Based on Measurements in a Noisy Environment
,”
J. Acoust. Soc. Am.
,
134
(
4
), pp.
2823
2832
.
19.
Bi
,
C. X.
, and
Bolton
,
J. S.
,
2012
, “
An Equivalent Source Technique for Recovering the Free Sound Field in a Noisy Environment
,”
J. Acoust. Soc. Am.
,
131
(
2
), pp.
1260
1270
.
20.
Stephenne
,
A.
, and
Champagne
,
B.
,
1997
, “
A New Cepstral Prefiltering Technique for Estimating Time Delay Under Reverberant Conditions
,”
Signal Process.
,
59
(
3
), pp.
253
266
.
21.
Benesty
,
J.
,
2000
, “
Adaptive Eigenvalue Decomposition Algorithm for Passive Acoustic Source Localization
,”
J. Acoust. Soc. Am.
,
107
(
1
), pp.
384
391
.
22.
Gover
,
B. N.
,
Ryan
,
J. G.
, and
Stinson
,
M. R.
,
2004
, “
Measurements of Directional Properties of Reverberant Sound Fields in Rooms Using a Spherical Microphone Array
,”
J. Acoust. Soc. Am.
,
116
(
4
), pp.
2138
2148
.
23.
Fisher
,
E.
, and
Rafaely
,
B.
,
2008
, “
The Nearfield Spherical Microphone Array
,”
IEEE
International Conference on Acoustics, Speech and Signal Processing
, Las Vegas, NV, Mar. 31–Apr. 4, pp.
5272
5275
.
24.
Fink
,
M.
,
Prada
,
C.
,
Wu
,
F.
, and
Cassereau
,
D.
,
1989
, “
Self Focusing in Inhomogeneous Media With Time Reversal Acoustic Mirrors
,”
IEEE
Ultrasonics Symposium Proceedings
, Montreal, QC, Canada, Oct. 3–6, pp.
681
686
.
25.
Fink
,
M.
,
1992
, “
Time Reversal of Ultrasonic Fields—Part I: Basic Principles
,”
IEEE Trans. Ultrason., Ferroelectr. Freq. Control
,
39
(
5
), pp.
555
566
.
26.
Bi
,
C. X.
,
Li
,
Y. C.
,
Zhang
,
Y. B.
, and
Xu
,
L.
,
2017
, “
Super-Resolution Imaging of Low-Frequency Sound Sources Using a Corrected Monopole Time Reversal Method
,”
J. Sound Vib.
,
410
, pp.
303
317
.
27.
Bi
,
C. X.
,
Li
,
Y. C.
,
Zhou
,
R.
, and
Zhang
,
Y. B.
,
2018
, “
A Comparison of Equivalent Source Method and Monopole Time Reversal Method for Noise Source Localization
,”
ASME J. Vib. Acoust.
,
140
(
6
), p.
061011
.
28.
Wu
,
B. H.
,
Too
,
G. P.
, and
Lee
,
S.
,
2010
, “
Audio Signal Separation Via a Combination Procedure of Time-Reversal and Deconvolution Process
,”
Mech. Syst. Signal Process.
,
24
(
5
), pp.
1431
1443
.
29.
Yon
,
S.
,
Tanter
,
M.
, and
Fink
,
M.
,
2003
, “
Sound Focusing in Rooms: The Time-Reversal Approach
,”
J. Acoust. Soc. Am.
,
113
(
3
), pp.
1533
1543
.
30.
Ribay
,
G.
,
de Rosny
,
J.
, and
Fink
,
M.
,
2005
, “
Time Reversal of Noise Sources in a Reverberation Room
,”
J. Acoust. Soc. Am.
,
117
(
5
), pp.
2866
2872
.
31.
Wei
,
L.
,
Li
,
M.
,
Yang
,
D. B.
,
Niu
,
F.
, and
Zeng
,
W.
,
2017
, “
Reconstruction of Sound Source Signal by Analytical Passive TR in the Environment With Airflow
,”
J. Sound Vib.
,
392
, pp.
77
90
.
32.
Druault
,
P.
,
Marchiano
,
R.
, and
Sagaut
,
P.
,
2013
, “
Localization of Aeroacoustic Sound Sources in Viscous Flows by a Time Reversal Method
,”
J. Sound Vib.
,
332
(
15
), pp.
3655
3669
.
33.
Vergnault
,
E.
,
Malaspinas
,
O.
, and
Sagaut
,
P.
,
2013
, “
Noise Source Identification With the Lattice Boltzmann Method
,”
J. Acoust. Soc. Am.
,
133
(
3
), pp.
1293
1305
.
34.
Padois
,
T.
,
Prax
,
C.
,
Valeau
,
V.
, and
Marx
,
D.
,
2012
, “
Experimental Localization of an Acoustic Sound Source in a Wind-Tunnel Flow by Using a Numerical Time-Reversal Technique
,”
J. Acoust. Soc. Am.
,
132
(
4
), pp.
2397
2407
.
35.
Johnson
,
M. E.
,
Elliott
,
S. J.
,
Baek
,
K. H.
, and
Garcia-Bonito
,
J.
,
1998
, “
An Equivalent Source Technique for Calculating the Sound Field Inside an Enclosure Containing Scattering Objects
,”
J. Acoust. Soc. Am.
,
104
(
3
), pp.
1221
1231
.
36.
Zhang
,
Y.
,
Zhang
,
X. Z.
,
Bi
,
C. X.
, and
Zhang
,
Y. B.
,
2017
, “
An Inverse Direct Time Domain Boundary Element Method for the Reconstruction of Transient Acoustic Field
,”
ASME J. Vib. Acoust.
,
139
(
2
), p.
021013
.
37.
Harker
,
B. M.
, and
Anderson
,
B. E.
,
2013
, “
Optimization of the Array Mirror for Time Reversal Techniques Used in a Half-Space Environment
,”
J. Acoust. Soc. Am.
,
133
(
5
), pp.
EL351
EL357
.
You do not currently have access to this content.