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Power output minimization and power absorption in the active control of sound

Power output minimization and power absorption in the active control of sound
Power output minimization and power absorption in the active control of sound

Active minimization of total power output and active absorption of sound power are analyzed, using a general impedance-based approach, for an array of controllable secondary sources and an array of original primary sources. When the total power output of the two arrays is minimized, and the primary source array is all in phase, the power output of each of the secondary sources is found to be exactly zero. When the power absorption of the secondary source array is maximized, the net power output of the primary source array can be either reduced or increased, compared to that in the absence of control, depending on the properties of the transfer impedances. If the primary and secondary sources are well coupled (as is the case when they are spaced less than a quarter wavelength apart in free-space or when they are in an enclosure excited near the natural frequency of a lightly damped mode) minimizing the total power output gives worthwhile reductions in the radiated power of the primary source. Maximizing the power absorption of the secondary source under these conditions, however, can considerably increase the power output of the primary source. If the sources are well separated, compared with the wavelength, in the free-field, or are placed in a diffuse sound field in an enclosure, the coupling between the sources is weak. Under these conditions the secondary source can effect little reduction in the power output of the primary source. Although acoustic power can still be absorbed by the secondary source under such circumstances, the amount of absorbed power will always be small compared with the power output of the primary source.

0001-4966
2501-2512
Elliotl, S. J.
fbfe93a9-5dc9-4839-b400-b0f811160fbc
Joseph, P.
9c30491e-8464-4c9a-8723-2abc62bdf75d
Nelson, P. A.
5c6f5cc9-ea52-4fe2-9edf-05d696b0c1a9
Johnson, M. E.
d781819a-c194-4f44-9daa-204375973038
Elliotl, S. J.
fbfe93a9-5dc9-4839-b400-b0f811160fbc
Joseph, P.
9c30491e-8464-4c9a-8723-2abc62bdf75d
Nelson, P. A.
5c6f5cc9-ea52-4fe2-9edf-05d696b0c1a9
Johnson, M. E.
d781819a-c194-4f44-9daa-204375973038

Elliotl, S. J., Joseph, P., Nelson, P. A. and Johnson, M. E. (1991) Power output minimization and power absorption in the active control of sound. Journal of the Acoustical Society of America, 90 (5), 2501-2512. (doi:10.1121/1.402054).

Record type: Article

Abstract

Active minimization of total power output and active absorption of sound power are analyzed, using a general impedance-based approach, for an array of controllable secondary sources and an array of original primary sources. When the total power output of the two arrays is minimized, and the primary source array is all in phase, the power output of each of the secondary sources is found to be exactly zero. When the power absorption of the secondary source array is maximized, the net power output of the primary source array can be either reduced or increased, compared to that in the absence of control, depending on the properties of the transfer impedances. If the primary and secondary sources are well coupled (as is the case when they are spaced less than a quarter wavelength apart in free-space or when they are in an enclosure excited near the natural frequency of a lightly damped mode) minimizing the total power output gives worthwhile reductions in the radiated power of the primary source. Maximizing the power absorption of the secondary source under these conditions, however, can considerably increase the power output of the primary source. If the sources are well separated, compared with the wavelength, in the free-field, or are placed in a diffuse sound field in an enclosure, the coupling between the sources is weak. Under these conditions the secondary source can effect little reduction in the power output of the primary source. Although acoustic power can still be absorbed by the secondary source under such circumstances, the amount of absorbed power will always be small compared with the power output of the primary source.

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More information

Published date: November 1991
Additional Information: Copyright: Copyright 2016 Elsevier B.V., All rights reserved.

Identifiers

Local EPrints ID: 468601
URI: http://eprints.soton.ac.uk/id/eprint/468601
ISSN: 0001-4966
PURE UUID: a27a5288-d9fa-4919-bec9-4e533b5c89d4
ORCID for P. A. Nelson: ORCID iD orcid.org/0000-0002-9563-3235

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Date deposited: 18 Aug 2022 16:42
Last modified: 17 Mar 2024 02:32

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Contributors

Author: S. J. Elliotl
Author: P. Joseph
Author: P. A. Nelson ORCID iD
Author: M. E. Johnson

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