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On the potential limitations of conventional sound metrics in quantifying perception of nonlinearly propagated noise

J. Acoust. Soc. Am. Volume 121, Issue 1, pp. EL1-EL7 (2006); (7 pages)

Kent L. Gee1, S. Hales Swift1, Victor W. Sparrow2, Kenneth J. Plotkin3, and J. Micah Downing4

1Department of Physics and Astronomy, N319 ESC, Brigham Young University, Provo, Utah 84602
2Graduate Program in Acoustics, 201 Applied Science Building, The Pennsylvania State University, University Park, Pennsylvania 16802
3Wyle Laboratories, 2001 Jefferson Davis Highway, Suite 701, Arlington, Virginia 22202
4Blue Ridge Research and Consulting, LLC, 13 1/2 West Walnut Street, Asheville, North Carolina 28801

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The use of conventional metrics to quantify the perception of nonlinearly propagated noise has been studied. Gaussian noise waveforms have been numerically propagated both linearly and nonlinearly, and from the resulting waveforms, several metrics are calculated. These metrics are overall, A-, C-, and D-weighted sound pressure levels, perceived noise level, Stevens Mark VII perceived loudness, Zwicker loudness, and sharpness. Informal listening demonstrations indicate that perceived differences in annoyance between linearly and nonlinearly propagated waveforms are substantial. Because the metrics studied seem inadequate in representing the perceived differences, rigorous subjective testing is encouraged to properly quantify and understand these differences.

© 2007 Acoustical Society of America

Acknowledgment

This work was supported in part by the Strategic Environmental Research and Development Program.

Article Outline

  1. Introduction
  2. Metrics considered
  3. Test case description and results
    1. Test case description
    2. Waveform playback
  4. Metric calculations and discussion
  5. Conclusion

KEYWORDS and PACS

PACS

  • 43.50.Ba

    Noisiness: rating methods and criteria

  • 43.66.Lj

    Perceptual effects of sound

  • 43.25.Cb

    Macrosonic propagation, finite amplitude sound; shock waves

ARTICLE DATA

History
Received 14 Aug 2006
Accepted 20 Oct 2006
Revised 19 Oct 2006
Published online 08 Dec 2006

PUBLICATION DATA

ISSN

0001-4966 (print)  

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Figures (1) Multimedia (4) Tables (1)

Figures (click on thumbnails to view enlargements)

FIG.1
(a) Input power spectral density at 10 m and predicted power spectral densities at 1000 m. (b) Short segments of the nonlinearly and linearly predicted waveforms at 1000 m as a function of retarded time, τ. Note the shock-like steepness of the nonlinearly predicted waveform at approximately 1.107 and 1.114 s.

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Multimedia

Tables

Table I. Calculated metrics and difference for the nonlinearly and linearly predicted waveforms. L denotes overall sound pressure level and the subscripts signify the type of weighting applied. PNL, PL, ZL, and S, respectively, represent perceived noise level, Stevens Mark VII perceived loudness, Zwicker loudness, and sharpness.

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